From 524b613f3f9018405cd2ed684216b2a2fd9662b8 Mon Sep 17 00:00:00 2001 From: Matthew Templeton Date: Thu, 18 Apr 2024 09:17:28 -0400 Subject: [PATCH 01/10] Adds msup tag to allowed MathML in base.py modified: adsingestp/parsers/base.py --- adsingestp/parsers/base.py | 1 + 1 file changed, 1 insertion(+) diff --git a/adsingestp/parsers/base.py b/adsingestp/parsers/base.py index 3659cd6..5ad0252 100644 --- a/adsingestp/parsers/base.py +++ b/adsingestp/parsers/base.py @@ -489,6 +489,7 @@ class BaseBeautifulSoupParser(IngestBase): "mml:mn", "mml:annotation", "mml:msubsup", + "mml:msup", ] HTML_TAGS_HTML = ["sub", "sup", "a", "astrobj", "i", "b"] From 711ec364e43385b9136474c72cc1e1de6c8115b2 Mon Sep 17 00:00:00 2001 From: Matthew Templeton Date: Thu, 18 Apr 2024 09:38:27 -0400 Subject: [PATCH 02/10] Uniform test output jsons (indent, sort_keys) modified: tests/stubdata/output/copernicus_ESSD_essd-15-3075-2023.json modified: tests/stubdata/output/copernicus_GeChr_gchron-5-323-2023.json modified: tests/stubdata/output/copernicus_ISPAn_isprs-annals-X-M-1-2023-237-2023.json modified: tests/stubdata/output/copernicus_ISPAr_isprs-archives-XLVIII-M-2-2023-721-2023.json modified: tests/stubdata/output/crossref_10.1002_1521-3994.json modified: tests/stubdata/output/crossref_10.1103_PhysRevD_64-117303.json modified: tests/stubdata/output/crossref_10.1146_annurev.energy.25.1.441.json modified: tests/stubdata/output/crossref_10.3137_a0410105.json modified: tests/stubdata/output/crossref_10.3847_2041-8213.json modified: tests/stubdata/output/crossref_book_10.1007-978-1-4614-3520-4.json modified: tests/stubdata/output/crossref_book_10.1017-CBO9780511709265.json modified: tests/stubdata/output/crossref_cn_10.1051=0004-6361=202243540.json modified: tests/stubdata/output/crossref_cn_10.1088=1475-7516=2022=10=098.json modified: tests/stubdata/output/crossref_cn_10.1093=mnras=stac2975.json modified: tests/stubdata/output/crossref_cn_10.1093=pasj=psac053.json modified: tests/stubdata/output/crossref_cn_10.3847=1538-4357=ac8c2f.json modified: tests/stubdata/output/crossref_conf_10.1049-cp.2010.1342.json modified: tests/stubdata/output/crossref_conf_10.1109-MWSYM.2013.6697399.json modified: tests/stubdata/output/crossref_preprint_10.1002-essoar.10508651.1.json modified: tests/stubdata/output/crossref_preprint_10.1002-essoar.10511074.2.json modified: tests/stubdata/output/crossref_preprint_10.31223-X55K7G.json modified: tests/stubdata/output/crossref_preprint_10.31223-X5FW25.json modified: tests/stubdata/output/crossref_preprint_10.31223-X5WD2C.json modified: tests/stubdata/output/datacite_schema3.1_example-full.json modified: tests/stubdata/output/datacite_schema4.1_example-full.json modified: tests/stubdata/output/datacite_schema4.1_example-software.json modified: tests/stubdata/output/datacite_schema4_example-habanero-pdsdataset.json modified: tests/stubdata/output/els_missing_keywords_tag.json modified: tests/stubdata/output/jats_a+a_multiparagraph_abstract.json modified: tests/stubdata/output/jats_a+a_subtitle.json modified: tests/stubdata/output/jats_aip_aipc_2470_040010.json modified: tests/stubdata/output/jats_aip_amjph_90_286.json modified: tests/stubdata/output/jats_aj_158_4_139.json modified: tests/stubdata/output/jats_aj_158_4_139_fulltext.json modified: tests/stubdata/output/jats_aj_158_4_139_fulltext_tags.json modified: tests/stubdata/output/jats_iop_aj_162_1.json modified: tests/stubdata/output/jats_iop_ansnn_12_2_025001.json modified: tests/stubdata/output/jats_iop_apj_923_1_47.json modified: tests/stubdata/output/jats_iop_no_contribs.json modified: tests/stubdata/output/jats_iop_no_orcid_tag.json modified: tests/stubdata/output/jats_iop_preprint_in_record.json modified: tests/stubdata/output/jats_mnras_493_1_141.json modified: tests/stubdata/output/jats_phrvd_106_023001.json modified: tests/stubdata/output/jats_pnas_1715554115.json modified: tests/stubdata/output/jats_spie_opten_1.OE.62.4.048103.json modified: tests/stubdata/output/jats_spie_opten_1.OE.62.4.066101.json modified: tests/stubdata/output/jats_spie_spie_12.2690579.json modified: tests/stubdata/output/jats_springer_EPJC_s10052-023-11699-1.json modified: tests/stubdata/output/jats_springer_EPJC_s10052-023-11733-2.json modified: tests/stubdata/output/jats_springer_NatCo_s41467-023-40272-3.json modified: tests/stubdata/output/jats_springer_Natur_s41598-023-38673-x.json modified: tests/stubdata/output/jats_springer_ZaMP_s00033-023-02064-z.json modified: tests/stubdata/output/wiley_jgra_12057.json modified: tests/stubdata/output/wiley_jgra_57392.json modified: tests/stubdata/output/wiley_swe_21103.json modified: tests/stubdata/output/wiley_swe_461.json modified: tests/stubdata/output/wiley_swe_539.json modified: tests/stubdata/output/zenodo_test.json modified: tests/stubdata/output/zenodo_test2.json modified: tests/stubdata/output/zenodo_test3.json modified: tests/stubdata/output/zenodo_test4.json --- .../copernicus_ESSD_essd-15-3075-2023.json | 490 +- .../copernicus_GeChr_gchron-5-323-2023.json | 140 +- ...SPAn_isprs-annals-X-M-1-2023-237-2023.json | 124 +- ...prs-archives-XLVIII-M-2-2023-721-2023.json | 132 +- .../output/crossref_10.1002_1521-3994.json | 82 +- .../crossref_10.1103_PhysRevD_64-117303.json | 92 +- ...ssref_10.1146_annurev.energy.25.1.441.json | 102 +- .../output/crossref_10.3137_a0410105.json | 104 +- .../output/crossref_10.3847_2041-8213.json | 136 +- ...ossref_book_10.1007-978-1-4614-3520-4.json | 96 +- ...rossref_book_10.1017-CBO9780511709265.json | 70 +- ...ossref_cn_10.1051=0004-6361=202243540.json | 116 +- ...sref_cn_10.1088=1475-7516=2022=10=098.json | 112 +- .../crossref_cn_10.1093=mnras=stac2975.json | 206 +- .../crossref_cn_10.1093=pasj=psac053.json | 166 +- .../crossref_cn_10.3847=1538-4357=ac8c2f.json | 164 +- .../crossref_conf_10.1049-cp.2010.1342.json | 80 +- ...ssref_conf_10.1109-MWSYM.2013.6697399.json | 138 +- ...ef_preprint_10.1002-essoar.10508651.1.json | 262 +- ...ef_preprint_10.1002-essoar.10511074.2.json | 170 +- .../crossref_preprint_10.31223-X55K7G.json | 118 +- .../crossref_preprint_10.31223-X5FW25.json | 190 +- .../crossref_preprint_10.31223-X5WD2C.json | 78 +- .../datacite_schema3.1_example-full.json | 134 +- .../datacite_schema4.1_example-full.json | 130 +- .../datacite_schema4.1_example-software.json | 154 +- ...e_schema4_example-habanero-pdsdataset.json | 134 +- .../output/els_missing_keywords_tag.json | 2 +- .../jats_a+a_multiparagraph_abstract.json | 494 +- tests/stubdata/output/jats_a+a_subtitle.json | 750 +- .../output/jats_aip_aipc_2470_040010.json | 218 +- .../output/jats_aip_amjph_90_286.json | 242 +- tests/stubdata/output/jats_aj_158_4_139.json | 422 +- .../output/jats_aj_158_4_139_fulltext.json | 22 +- .../jats_aj_158_4_139_fulltext_tags.json | 17 +- tests/stubdata/output/jats_iop_aj_162_1.json | 244 +- .../output/jats_iop_ansnn_12_2_025001.json | 272 +- .../output/jats_iop_apj_923_1_47.json | 318 +- .../stubdata/output/jats_iop_no_contribs.json | 82 +- .../output/jats_iop_no_orcid_tag.json | 5284 +-- .../output/jats_iop_preprint_in_record.json | 186 +- .../stubdata/output/jats_mnras_493_1_141.json | 326 +- .../output/jats_phrvd_106_023001.json | 276 +- .../stubdata/output/jats_pnas_1715554115.json | 3216 +- .../jats_spie_opten_1.OE.62.4.048103.json | 200 +- .../jats_spie_opten_1.OE.62.4.066101.json | 194 +- .../output/jats_spie_spie_12.2690579.json | 134 +- ...jats_springer_EPJC_s10052-023-11699-1.json | 36752 ++++++++-------- ...jats_springer_EPJC_s10052-023-11733-2.json | 17722 ++++---- ...ats_springer_NatCo_s41467-023-40272-3.json | 722 +- ...ats_springer_Natur_s41598-023-38673-x.json | 850 +- ...jats_springer_ZaMP_s00033-023-02064-z.json | 256 +- tests/stubdata/output/wiley_jgra_12057.json | 193 +- tests/stubdata/output/wiley_jgra_57392.json | 329 +- tests/stubdata/output/wiley_swe_21103.json | 441 +- tests/stubdata/output/wiley_swe_461.json | 74 +- tests/stubdata/output/wiley_swe_539.json | 74 +- tests/stubdata/output/zenodo_test.json | 92 +- tests/stubdata/output/zenodo_test2.json | 330 +- tests/stubdata/output/zenodo_test3.json | 262 +- tests/stubdata/output/zenodo_test4.json | 134 +- 61 files changed, 37882 insertions(+), 37168 deletions(-) diff --git a/tests/stubdata/output/copernicus_ESSD_essd-15-3075-2023.json b/tests/stubdata/output/copernicus_ESSD_essd-15-3075-2023.json index 8e2137d..c101c5d 100644 --- a/tests/stubdata/output/copernicus_ESSD_essd-15-3075-2023.json +++ b/tests/stubdata/output/copernicus_ESSD_essd-15-3075-2023.json @@ -1,48 +1,9 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2023-07-20", - "printDate": "2023-07-20" - }, - "publication": { - "pubName": "Earth System Science Data", - "volumeNum": "15", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "print", - "issnString": "1866-3508" - }, - { - "pubtype": "electronic", - "issnString": "1866-3516" - } - ] - }, - "pagination": { - "electronicID": "145", - "firstPage": "3075", - "lastPage": "3094" + "abstract": { + "textEnglish": "Saharan dust outbreaks have profound effects on ecosystems, climate, human health, and the cryosphere in Europe. However, the spatial deposition pattern of Saharan dust is poorly known due to a sparse network of ground measurements. Following the extreme dust deposition event of February 2021 across Europe, a citizen science campaign was launched to sample dust on snow over the Pyrenees and the European Alps. This somewhat improvised campaign triggered wide interest since 152 samples were collected from the snow in the Pyrenees, the French Alps, and the Swiss Alps in less than 4 weeks. Among the 152 samples, 113 in total could be analysed, corresponding to 70 different locations. The analysis of the samples showed a large variability in the dust properties and amount. We found a decrease in the deposited mass and particle sizes with distance from the source along the transport path. This spatial trend was also evident in the elemental composition of the dust as the iron mass fraction decreased from 11 % in the Pyrenees to 2 % in the Swiss Alps. At the local scale, we found a higher dust mass on south-facing slopes, in agreement with estimates from high-resolution remote sensing data. This unique dataset, which resulted from the collaboration of several research laboratories and citizens, is provided as an open dataset to benefit a large community and to enable further scientific investigations. Data presented in this study are available at https://doi.org/10.5281/zenodo.7969515 (Dumont et al., 2022a)." }, - "persistentIDs": [ - { - "DOI": "10.5194/essd-15-3075-2023" - } - ], "authors": [ { - "name": { - "surname": "Dumont", - "given_name": "Marie", - "pubraw": "Marie Dumont" - }, "affiliation": [ { "affPubRaw": "Univ. Grenoble Alpes, Universit\u00e9 de Toulouse, M\u00e9t\u00e9o-France, CNRS, CNRM, Centre d\u2019\u00c9tudes de la Neige, 38000 Grenoble, France" @@ -51,14 +12,14 @@ "attrib": { "email": "marie.dumont@meteo.fr", "orcid": "0000-0002-4002-5873" + }, + "name": { + "given_name": "Marie", + "pubraw": "Marie Dumont", + "surname": "Dumont" } }, { - "name": { - "surname": "Gascoin", - "given_name": "Simon", - "pubraw": "Simon Gascoin" - }, "affiliation": [ { "affPubRaw": "CESBIO, Universit\u00e9 de Toulouse, CNES/CNRS/INRA/IRD/UPS, Toulouse, France" @@ -67,14 +28,14 @@ "attrib": { "email": "sgascoin@gmail.com", "orcid": "0000-0002-4996-6768" + }, + "name": { + "given_name": "Simon", + "pubraw": "Simon Gascoin", + "surname": "Gascoin" } }, { - "name": { - "surname": "R\u00e9veillet", - "given_name": "Marion", - "pubraw": "Marion R\u00e9veillet" - }, "affiliation": [ { "affPubRaw": "Univ. Grenoble Alpes, Universit\u00e9 de Toulouse, M\u00e9t\u00e9o-France, CNRS, CNRM, Centre d\u2019\u00c9tudes de la Neige, 38000 Grenoble, France" @@ -86,14 +47,14 @@ "attrib": { "email": "marion.reveillet@univ-grenoble-alpes.fr", "orcid": "0000-0001-9802-4649" + }, + "name": { + "given_name": "Marion", + "pubraw": "Marion R\u00e9veillet", + "surname": "R\u00e9veillet" } }, { - "name": { - "surname": "Voisin", - "given_name": "Didier", - "pubraw": "Didier Voisin" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 Grenoble Alpes, CNRS, IRD, G-INP, IGE, Grenoble, France" @@ -102,14 +63,14 @@ "attrib": { "email": "didier.voisin@univ-grenoble-alpes.fr", "orcid": "0000-0003-1317-7561" + }, + "name": { + "given_name": "Didier", + "pubraw": "Didier Voisin", + "surname": "Voisin" } }, { - "name": { - "surname": "Tuzet", - "given_name": "Fran\u00e7ois", - "pubraw": "Fran\u00e7ois Tuzet" - }, "affiliation": [ { "affPubRaw": "Univ. Grenoble Alpes, Universit\u00e9 de Toulouse, M\u00e9t\u00e9o-France, CNRS, CNRM, Centre d\u2019\u00c9tudes de la Neige, 38000 Grenoble, France" @@ -117,14 +78,14 @@ ], "attrib": { "email": "francois.tuzet@gmail.com" + }, + "name": { + "given_name": "Fran\u00e7ois", + "pubraw": "Fran\u00e7ois Tuzet", + "surname": "Tuzet" } }, { - "name": { - "surname": "Arnaud", - "given_name": "Laurent", - "pubraw": "Laurent Arnaud" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 Grenoble Alpes, CNRS, IRD, G-INP, IGE, Grenoble, France" @@ -133,14 +94,14 @@ "attrib": { "email": "laurent.arnaud@univ-grenoble-alpes.fr", "orcid": "0000-0002-4432-4205" + }, + "name": { + "given_name": "Laurent", + "pubraw": "Laurent Arnaud", + "surname": "Arnaud" } }, { - "name": { - "surname": "Bonnefoy", - "given_name": "Myl\u00e8ne", - "pubraw": "Myl\u00e8ne Bonnefoy" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 Grenoble Alpes, INRAE, UR ETGR, Grenoble, France" @@ -148,14 +109,14 @@ ], "attrib": { "email": "mylene.bonnefoy@inrae.fr" + }, + "name": { + "given_name": "Myl\u00e8ne", + "pubraw": "Myl\u00e8ne Bonnefoy", + "surname": "Bonnefoy" } }, { - "name": { - "surname": "Bacardit Pe\u00f1arroya", - "given_name": "Montse", - "pubraw": "Montse Bacardit Pe\u00f1arroya" - }, "affiliation": [ { "affPubRaw": "Centre de Lauegi d'Aran, Conselh Generau d'Aran, Viella, Spain" @@ -163,14 +124,14 @@ ], "attrib": { "email": "m.bacardit@aran.org" + }, + "name": { + "given_name": "Montse", + "pubraw": "Montse Bacardit Pe\u00f1arroya", + "surname": "Bacardit Pe\u00f1arroya" } }, { - "name": { - "surname": "Carmagnola", - "given_name": "Carlo", - "pubraw": "Carlo Carmagnola" - }, "affiliation": [ { "affPubRaw": "Univ. Grenoble Alpes, Universit\u00e9 de Toulouse, M\u00e9t\u00e9o-France, CNRS, CNRM, Centre d\u2019\u00c9tudes de la Neige, 38000 Grenoble, France" @@ -178,14 +139,14 @@ ], "attrib": { "email": "carlo.carmagnola@meteo.fr" + }, + "name": { + "given_name": "Carlo", + "pubraw": "Carlo Carmagnola", + "surname": "Carmagnola" } }, { - "name": { - "surname": "Deguine", - "given_name": "Alexandre", - "pubraw": "Alexandre Deguine" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 de Lille, CNRS, UMR 8518 \u2013 LOA \u2013 Laboratoire d'Optique Atmosph\u00e9rique, 59000 Lille, France" @@ -197,14 +158,14 @@ "attrib": { "email": "alexandre.deguine@univ-lille.fr", "orcid": "0000-0001-7125-3759" + }, + "name": { + "given_name": "Alexandre", + "pubraw": "Alexandre Deguine", + "surname": "Deguine" } }, { - "name": { - "surname": "Diacre", - "given_name": "Aur\u00e9lie", - "pubraw": "Aur\u00e9lie Diacre" - }, "affiliation": [ { "affPubRaw": "Commissariat \u00c0 L\u2019Energie Atomique Et aux \u00c9nergies Alternatives (CEA, DAM, DIF), 91297 Arpajon, France" @@ -213,14 +174,14 @@ "attrib": { "email": "aurelie.diacre@lsce.ipsl.fr", "orcid": "0000-0001-6988-1828" + }, + "name": { + "given_name": "Aur\u00e9lie", + "pubraw": "Aur\u00e9lie Diacre", + "surname": "Diacre" } }, { - "name": { - "surname": "D\u00fcrr", - "given_name": "Lukas", - "pubraw": "Lukas D\u00fcrr" - }, "affiliation": [ { "affPubRaw": "WSL Institute for Snow and Avalanche Research SLF, Fl\u00fcelastr. 11, 7260 Davos, Switzerland" @@ -228,14 +189,14 @@ ], "attrib": { "email": "duerr@slf.ch" + }, + "name": { + "given_name": "Lukas", + "pubraw": "Lukas D\u00fcrr", + "surname": "D\u00fcrr" } }, { - "name": { - "surname": "Evrard", - "given_name": "Olivier", - "pubraw": "Olivier Evrard" - }, "affiliation": [ { "affPubRaw": "LSCE \u2013 IPSL \u2013 Laboratoire des Sciences du Climat et de l'Environnement, CEA, CNRS, UVSQ, Universit\u00e9 Paris-Saclay, Gif-sur-Yvette, France" @@ -244,14 +205,14 @@ "attrib": { "email": "olivier.evrard@lsce.ipsl.fr", "orcid": "0000-0002-3503-6543" + }, + "name": { + "given_name": "Olivier", + "pubraw": "Olivier Evrard", + "surname": "Evrard" } }, { - "name": { - "surname": "Fontaine", - "given_name": "Firmin", - "pubraw": "Firmin Fontaine" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 Grenoble Alpes, INRAE, UR ETGR, Grenoble, France" @@ -259,14 +220,14 @@ ], "attrib": { "email": "firmin.fontaine@inrae.fr" + }, + "name": { + "given_name": "Firmin", + "pubraw": "Firmin Fontaine", + "surname": "Fontaine" } }, { - "name": { - "surname": "Frankl", - "given_name": "Amaury", - "pubraw": "Amaury Frankl" - }, "affiliation": [ { "affPubRaw": "INRAE, AMAP, IRD, CIRAD, CNRS, University Montpellier, Bld de la Lironde, 34398, Montpellier CEDEX 5, France" @@ -278,14 +239,14 @@ "attrib": { "email": "amaury.frankl@ugent.be", "orcid": "0000-0002-1685-2780" + }, + "name": { + "given_name": "Amaury", + "pubraw": "Amaury Frankl", + "surname": "Frankl" } }, { - "name": { - "surname": "Fructus", - "given_name": "Mathieu", - "pubraw": "Mathieu Fructus" - }, "affiliation": [ { "affPubRaw": "Univ. Grenoble Alpes, Universit\u00e9 de Toulouse, M\u00e9t\u00e9o-France, CNRS, CNRM, Centre d\u2019\u00c9tudes de la Neige, 38000 Grenoble, France" @@ -293,14 +254,14 @@ ], "attrib": { "email": "mathieu.fructus@meteo.fr" + }, + "name": { + "given_name": "Mathieu", + "pubraw": "Mathieu Fructus", + "surname": "Fructus" } }, { - "name": { - "surname": "Gandois", - "given_name": "Laure", - "pubraw": "Laure Gandois" - }, "affiliation": [ { "affPubRaw": "Laboratoire Ecologie Fonctionnelle et Environnement, Universit\u00e9 de Toulouse, CNRS, INPT, UPS, Toulouse, France" @@ -308,14 +269,14 @@ ], "attrib": { "email": "laure.gandois@toulouse-inp.fr" + }, + "name": { + "given_name": "Laure", + "pubraw": "Laure Gandois", + "surname": "Gandois" } }, { - "name": { - "surname": "Gouttevin", - "given_name": "Isabelle", - "pubraw": "Isabelle Gouttevin" - }, "affiliation": [ { "affPubRaw": "Univ. Grenoble Alpes, Universit\u00e9 de Toulouse, M\u00e9t\u00e9o-France, CNRS, CNRM, Centre d\u2019\u00c9tudes de la Neige, 38000 Grenoble, France" @@ -324,14 +285,14 @@ "attrib": { "email": "isabelle.gouttevin@meteo.fr", "orcid": "0000-0002-1801-684X" + }, + "name": { + "given_name": "Isabelle", + "pubraw": "Isabelle Gouttevin", + "surname": "Gouttevin" } }, { - "name": { - "surname": "Gherab", - "given_name": "Abdelfateh", - "pubraw": "Abdelfateh Gherab" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 Grenoble Alpes, CNRS, IRD, G-INP, IGE, Grenoble, France" @@ -339,14 +300,14 @@ ], "attrib": { "email": "abdelfateh.gherab@gmail.com" + }, + "name": { + "given_name": "Abdelfateh", + "pubraw": "Abdelfateh Gherab", + "surname": "Gherab" } }, { - "name": { - "surname": "Hagenmuller", - "given_name": "Pascal", - "pubraw": "Pascal Hagenmuller" - }, "affiliation": [ { "affPubRaw": "Univ. Grenoble Alpes, Universit\u00e9 de Toulouse, M\u00e9t\u00e9o-France, CNRS, CNRM, Centre d\u2019\u00c9tudes de la Neige, 38000 Grenoble, France" @@ -355,14 +316,14 @@ "attrib": { "email": "pascal.hagenmuller@meteo.fr", "orcid": "0000-0002-6581-2048" + }, + "name": { + "given_name": "Pascal", + "pubraw": "Pascal Hagenmuller", + "surname": "Hagenmuller" } }, { - "name": { - "surname": "Hansson", - "given_name": "Sophia", - "pubraw": "Sophia Hansson" - }, "affiliation": [ { "affPubRaw": "Laboratoire Ecologie Fonctionnelle et Environnement, Universit\u00e9 de Toulouse, CNRS, INPT, UPS, Toulouse, France" @@ -370,14 +331,14 @@ ], "attrib": { "email": "sophia.hansson@toulouse-inp.fr" + }, + "name": { + "given_name": "Sophia", + "pubraw": "Sophia Hansson", + "surname": "Hansson" } }, { - "name": { - "surname": "Herbin", - "given_name": "Herv\u00e9", - "pubraw": "Herv\u00e9 Herbin" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 de Lille, CNRS, UMR 8518 \u2013 LOA \u2013 Laboratoire d'Optique Atmosph\u00e9rique, 59000 Lille, France" @@ -385,14 +346,14 @@ ], "attrib": { "email": "herve.herbin@univ-lille.fr" + }, + "name": { + "given_name": "Herv\u00e9", + "pubraw": "Herv\u00e9 Herbin", + "surname": "Herbin" } }, { - "name": { - "surname": "Josse", - "given_name": "B\u00e9atrice", - "pubraw": "B\u00e9atrice Josse" - }, "affiliation": [ { "affPubRaw": "CNRM, Universit\u00e9 de Toulouse, M\u00e9t\u00e9o-France, CNRS, Toulouse, France" @@ -400,14 +361,14 @@ ], "attrib": { "email": "beatrice.josse@meteo.fr" + }, + "name": { + "given_name": "B\u00e9atrice", + "pubraw": "B\u00e9atrice Josse", + "surname": "Josse" } }, { - "name": { - "surname": "Jourdain", - "given_name": "Bruno", - "pubraw": "Bruno Jourdain" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 Grenoble Alpes, CNRS, IRD, G-INP, IGE, Grenoble, France" @@ -415,14 +376,14 @@ ], "attrib": { "email": "bruno.jourdain@univ-grenoble-alpes.fr" + }, + "name": { + "given_name": "Bruno", + "pubraw": "Bruno Jourdain", + "surname": "Jourdain" } }, { - "name": { - "surname": "Lefevre", - "given_name": "Irene", - "pubraw": "Irene Lefevre" - }, "affiliation": [ { "affPubRaw": "LSCE \u2013 IPSL \u2013 Laboratoire des Sciences du Climat et de l'Environnement, CEA, CNRS, UVSQ, Universit\u00e9 Paris-Saclay, Gif-sur-Yvette, France" @@ -430,14 +391,14 @@ ], "attrib": { "email": "irene.lefevre@lsce.ipsl.fr" + }, + "name": { + "given_name": "Irene", + "pubraw": "Irene Lefevre", + "surname": "Lefevre" } }, { - "name": { - "surname": "Le Roux", - "given_name": "Ga\u00ebl", - "pubraw": "Ga\u00ebl Le Roux" - }, "affiliation": [ { "affPubRaw": "Laboratoire Ecologie Fonctionnelle et Environnement, Universit\u00e9 de Toulouse, CNRS, INPT, UPS, Toulouse, France" @@ -446,14 +407,14 @@ "attrib": { "email": "gael.leroux@ensat.fr", "orcid": "0000-0002-1579-0178" + }, + "name": { + "given_name": "Ga\u00ebl", + "pubraw": "Ga\u00ebl Le Roux", + "surname": "Le Roux" } }, { - "name": { - "surname": "Libois", - "given_name": "Quentin", - "pubraw": "Quentin Libois" - }, "affiliation": [ { "affPubRaw": "CNRM, Universit\u00e9 de Toulouse, M\u00e9t\u00e9o-France, CNRS, Toulouse, France" @@ -462,14 +423,14 @@ "attrib": { "email": "quentin.libois@meteo.fr", "orcid": "0000-0001-8963-4170" + }, + "name": { + "given_name": "Quentin", + "pubraw": "Quentin Libois", + "surname": "Libois" } }, { - "name": { - "surname": "Liger", - "given_name": "Lucie", - "pubraw": "Lucie Liger" - }, "affiliation": [ { "affPubRaw": "Jardin du Lautaret, CNRS, Universit\u00e9 Grenoble Alpes, Grenoble, France" @@ -477,14 +438,14 @@ ], "attrib": { "email": "lucie.liger@univ-grenoble-alpes.fr" + }, + "name": { + "given_name": "Lucie", + "pubraw": "Lucie Liger", + "surname": "Liger" } }, { - "name": { - "surname": "Morin", - "given_name": "Samuel", - "pubraw": "Samuel Morin" - }, "affiliation": [ { "affPubRaw": "CNRM, Universit\u00e9 de Toulouse, M\u00e9t\u00e9o-France, CNRS, Toulouse, France" @@ -493,14 +454,14 @@ "attrib": { "email": "samuel.morin@meteo.fr", "orcid": "0000-0002-1781-687X" + }, + "name": { + "given_name": "Samuel", + "pubraw": "Samuel Morin", + "surname": "Morin" } }, { - "name": { - "surname": "Petitprez", - "given_name": "Denis", - "pubraw": "Denis Petitprez" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 de Lille, CNRS, UMR 8522 \u2013 PC2A \u2013 Physicochimie des Processus de Combustion et de l\u2019Atmosph\u00e8re, 59000 Lille, France" @@ -508,14 +469,14 @@ ], "attrib": { "email": "denis.petitprez@univ-lille.fr" + }, + "name": { + "given_name": "Denis", + "pubraw": "Denis Petitprez", + "surname": "Petitprez" } }, { - "name": { - "surname": "Robledano", - "given_name": "Alvaro", - "pubraw": "Alvaro Robledano" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 Grenoble Alpes, CNRS, IRD, G-INP, IGE, Grenoble, France" @@ -527,14 +488,14 @@ "attrib": { "email": "alvaro.robledano-perez@univ-grenoble-alpes.fr", "orcid": "0000-0002-4046-7065" + }, + "name": { + "given_name": "Alvaro", + "pubraw": "Alvaro Robledano", + "surname": "Robledano" } }, { - "name": { - "surname": "Schneebeli", - "given_name": "Martin", - "pubraw": "Martin Schneebeli" - }, "affiliation": [ { "affPubRaw": "WSL Institute for Snow and Avalanche Research SLF, Fl\u00fcelastr. 11, 7260 Davos, Switzerland" @@ -543,14 +504,14 @@ "attrib": { "email": "schneebeli@slf.ch", "orcid": "0000-0003-2872-4409" + }, + "name": { + "given_name": "Martin", + "pubraw": "Martin Schneebeli", + "surname": "Schneebeli" } }, { - "name": { - "surname": "Salze", - "given_name": "Pascal", - "pubraw": "Pascal Salze" - }, "affiliation": [ { "affPubRaw": "Jardin du Lautaret, CNRS, Universit\u00e9 Grenoble Alpes, Grenoble, France" @@ -558,14 +519,14 @@ ], "attrib": { "email": "pascal.salze@univ-grenoble-alpes.fr" + }, + "name": { + "given_name": "Pascal", + "pubraw": "Pascal Salze", + "surname": "Salze" } }, { - "name": { - "surname": "Six", - "given_name": "Delphine", - "pubraw": "Delphine Six" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 Grenoble Alpes, CNRS, IRD, G-INP, IGE, Grenoble, France" @@ -573,14 +534,14 @@ ], "attrib": { "email": "delphine.six@univ-grenoble-alpes.fr" + }, + "name": { + "given_name": "Delphine", + "pubraw": "Delphine Six", + "surname": "Six" } }, { - "name": { - "surname": "Thibert", - "given_name": "Emmanuel", - "pubraw": "Emmanuel Thibert" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 Grenoble Alpes, INRAE, UR ETGR, Grenoble, France" @@ -589,14 +550,14 @@ "attrib": { "email": "emmanuel.thibert@inrae.fr", "orcid": "0000-0003-2843-5367" + }, + "name": { + "given_name": "Emmanuel", + "pubraw": "Emmanuel Thibert", + "surname": "Thibert" } }, { - "name": { - "surname": "Trachsel", - "given_name": "J\u00fcrg", - "pubraw": "J\u00fcrg Trachsel" - }, "affiliation": [ { "affPubRaw": "WSL Institute for Snow and Avalanche Research SLF, Fl\u00fcelastr. 11, 7260 Davos, Switzerland" @@ -605,14 +566,14 @@ "attrib": { "email": "juerg.trachsel@slf.ch", "orcid": "0000-0003-2560-9907" + }, + "name": { + "given_name": "J\u00fcrg", + "pubraw": "J\u00fcrg Trachsel", + "surname": "Trachsel" } }, { - "name": { - "surname": "Vernay", - "given_name": "Matthieu", - "pubraw": "Matthieu Vernay" - }, "affiliation": [ { "affPubRaw": "Univ. Grenoble Alpes, Universit\u00e9 de Toulouse, M\u00e9t\u00e9o-France, CNRS, CNRM, Centre d\u2019\u00c9tudes de la Neige, 38000 Grenoble, France" @@ -620,14 +581,14 @@ ], "attrib": { "email": "matthieu.vernay@meteo.fr" + }, + "name": { + "given_name": "Matthieu", + "pubraw": "Matthieu Vernay", + "surname": "Vernay" } }, { - "name": { - "surname": "Viallon-Galinier", - "given_name": "L\u00e9o", - "pubraw": "L\u00e9o Viallon-Galinier" - }, "affiliation": [ { "affPubRaw": "Univ. Grenoble Alpes, Universit\u00e9 de Toulouse, M\u00e9t\u00e9o-France, CNRS, CNRM, Centre d\u2019\u00c9tudes de la Neige, 38000 Grenoble, France" @@ -635,14 +596,14 @@ ], "attrib": { "email": "leo.viallon@meteo.fr" + }, + "name": { + "given_name": "L\u00e9o", + "pubraw": "L\u00e9o Viallon-Galinier", + "surname": "Viallon-Galinier" } }, { - "name": { - "surname": "Voiron", - "given_name": "C\u00e9line", - "pubraw": "C\u00e9line Voiron" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 Grenoble Alpes, CNRS, IRD, G-INP, IGE, Grenoble, France" @@ -650,14 +611,60 @@ ], "attrib": { "email": "celine.voiron@ird.fr" + }, + "name": { + "given_name": "C\u00e9line", + "pubraw": "C\u00e9line Voiron", + "surname": "Voiron" } } ], - "title": { - "textEnglish": "Spatial Variability Of Saharan Dust Deposition Revealed Through A Citizen Science Campaign" + "esources": [ + { + "location": "https://essd.copernicus.org/articles/15/3075/2023/essd-15-3075-2023.pdf", + "source": "pub_pdf" + }, + { + "location": "https://essd.copernicus.org/articles/15/3075/2023/essd-15-3075-2023.html", + "source": "pub_html" + } + ], + "pagination": { + "electronicID": "145", + "firstPage": "3075", + "lastPage": "3094" }, - "abstract": { - "textEnglish": "Saharan dust outbreaks have profound effects on ecosystems, climate, human health, and the cryosphere in Europe. However, the spatial deposition pattern of Saharan dust is poorly known due to a sparse network of ground measurements. Following the extreme dust deposition event of February 2021 across Europe, a citizen science campaign was launched to sample dust on snow over the Pyrenees and the European Alps. This somewhat improvised campaign triggered wide interest since 152 samples were collected from the snow in the Pyrenees, the French Alps, and the Swiss Alps in less than 4 weeks. Among the 152 samples, 113 in total could be analysed, corresponding to 70 different locations. The analysis of the samples showed a large variability in the dust properties and amount. We found a decrease in the deposited mass and particle sizes with distance from the source along the transport path. This spatial trend was also evident in the elemental composition of the dust as the iron mass fraction decreased from 11 % in the Pyrenees to 2 % in the Swiss Alps. At the local scale, we found a higher dust mass on south-facing slopes, in agreement with estimates from high-resolution remote sensing data. This unique dataset, which resulted from the collaboration of several research laboratories and citizens, is provided as an open dataset to benefit a large community and to enable further scientific investigations. Data presented in this study are available at https://doi.org/10.5281/zenodo.7969515 (Dumont et al., 2022a)." + "persistentIDs": [ + { + "DOI": "10.5194/essd-15-3075-2023" + } + ], + "pubDate": { + "electrDate": "2023-07-20", + "printDate": "2023-07-20" + }, + "publication": { + "ISSN": [ + { + "issnString": "1866-3508", + "pubtype": "print" + }, + { + "issnString": "1866-3516", + "pubtype": "electronic" + } + ], + "pubName": "Earth System Science Data", + "pubYear": "2023", + "volumeNum": "15" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ "Adebiyi, A., Kok, J. F., Murray, B. J., Ryder, C. L., Stuut, J.-B. W., Kahn, R. A., Knippertz, P., Formenti, P., Mahowald, N. M., P\u00e9rez Garc\u00eda-Pando, C., Klose, M., Ansmann, A., Samset, B. H., Ito, A., Balkanski, Y., Di Biagio, C., Romanias, M. N., Huang, Y., and Meng, J.: A review of coarse mineral dust in the Earth system, Aeolian Res., 60, 100849, https://doi.org/10.1016/j.aeolia.2022.100849, 2023.\u2002a", @@ -710,14 +717,7 @@ "Vernay, M., Lafaysse, M., Monteiro, D., Hagenmuller, P., Nheili, R., Samaco\u00efts, R., Verfaillie, D., and Morin, S.: The S2M meteorological and snow cover reanalysis over the French mountainous areas: description and evaluation (1958\u20132021), Earth Syst. Sci. Data, 14, 1707\u20131733, https://doi.org/10.5194/essd-14-1707-2022, 2022. \u2002a", "Yu, H., Chin, M., Yuan, T., Bian, H., Remer, L. A., Prospero, J. M., Omar, A., Winker, D., Yang, Y., Zhang, Y., Zhang, Z., and Zhao, C.: The fertilizing role of African dust in the Amazon rainforest: A first multiyear assessment based on data from Cloud-Aerosol Lidar and Infrared Pathfinder Satellite Observations, Geophys. Res. Lett., 42, 1984\u20131991, https://doi.org/10.1002/2015GL063040, 2015.\u2002a" ], - "esources": [ - { - "source": "pub_pdf", - "location": "https://essd.copernicus.org/articles/15/3075/2023/essd-15-3075-2023.pdf" - }, - { - "source": "pub_html", - "location": "https://essd.copernicus.org/articles/15/3075/2023/essd-15-3075-2023.html" - } - ] + "title": { + "textEnglish": "Spatial Variability Of Saharan Dust Deposition Revealed Through A Citizen Science Campaign" + } } diff --git a/tests/stubdata/output/copernicus_GeChr_gchron-5-323-2023.json b/tests/stubdata/output/copernicus_GeChr_gchron-5-323-2023.json index 82dea0b..075160d 100644 --- a/tests/stubdata/output/copernicus_GeChr_gchron-5-323-2023.json +++ b/tests/stubdata/output/copernicus_GeChr_gchron-5-323-2023.json @@ -1,48 +1,9 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2023-07-19", - "printDate": "2023-07-19" - }, - "publication": { - "pubName": "Geochronology", - "volumeNum": "5", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "print", - "issnString": "2628-3697" - }, - { - "pubtype": "electronic", - "issnString": "2628-3719" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.5194/gchron-5-323-2023" - } - ], - "pagination": { - "electronicID": "18", - "firstPage": "323", - "lastPage": "332" + "abstract": { + "textEnglish": "In situ U\u2013Th\u2013He geochronology is a potentially disruptive technique that combines laser ablation inductively coupled plasma mass spectrometry (LA-ICP-MS) with laser microprobe noble gas mass spectrometry. Despite its potential to revolutionize (detrital) thermochronology, in situ U\u2013Th\u2013He dating is not widely used due to persistent analytical challenges. A major issue is that current in situ U\u2013Th\u2013He dating approaches require that the U, Th, and He measurements are expressed in units of molar concentration, in contrast with conventional methods, which use units of molar abundance. Whereas molar abundances can be reliably determined by isotope dilution, accurate concentration measurements are not so easy to obtain. In the absence of matrix-matched U\u2013Th concentration standards and accurate He ablation pit measurements, the required molar concentration calculations introduce an uncertainty that is higher than the conventional method, an uncertainty that is itself difficult to accurately quantify. We present a solution to this problem by using proton-induced 3He as a proxy for ablation pit volume and by pairing samples with a standard of known U\u2013Th\u2013He age. Thus, the U\u2013Th\u2013He age equation can be solved using relative rather than absolute concentration measurements. Pilot experiments show that the new method produces accurate results. However, it is prone to overdispersion, which is attributed to gradients in the proton fluence. These gradients can be measured, and their effect can be removed by fixing the geometry of the sample and the standard during the proton irradiation." }, "authors": [ { - "name": { - "surname": "Vermeesch", - "given_name": "Pieter", - "pubraw": "Pieter Vermeesch" - }, "affiliation": [ { "affPubRaw": "London Geochronology Centre, Department of Earth Sciences, University College London, Gower Street, London WC1E 6BT, UK" @@ -51,14 +12,14 @@ "attrib": { "email": "p.vermeesch@ucl.ac.uk", "orcid": "0000-0003-3404-1209" + }, + "name": { + "given_name": "Pieter", + "pubraw": "Pieter Vermeesch", + "surname": "Vermeesch" } }, { - "name": { - "surname": "Tian", - "given_name": "Yuntao", - "pubraw": "Yuntao Tian" - }, "affiliation": [ { "affPubRaw": "London Geochronology Centre, Department of Earth Sciences, University College London, Gower Street, London WC1E 6BT, UK" @@ -69,14 +30,14 @@ ], "attrib": { "email": "tianyuntao@mail.sysu.edu.cn" + }, + "name": { + "given_name": "Yuntao", + "pubraw": "Yuntao Tian", + "surname": "Tian" } }, { - "name": { - "surname": "Schwanethal", - "given_name": "Jae", - "pubraw": "Jae Schwanethal" - }, "affiliation": [ { "affPubRaw": "London Geochronology Centre, Department of Earth Sciences, University College London, Gower Street, London WC1E 6BT, UK" @@ -84,14 +45,14 @@ ], "attrib": { "email": "schwana@gmail.com" + }, + "name": { + "given_name": "Jae", + "pubraw": "Jae Schwanethal", + "surname": "Schwanethal" } }, { - "name": { - "surname": "Buret", - "given_name": "Yannick", - "pubraw": "Yannick Buret" - }, "affiliation": [ { "affPubRaw": "Department of Earth Sciences, Natural History Museum, Cromwell Road, London SW7 5BD, UK" @@ -99,14 +60,60 @@ ], "attrib": { "email": "y.buret@nhm.ac.uk" + }, + "name": { + "given_name": "Yannick", + "pubraw": "Yannick Buret", + "surname": "Buret" } } ], - "title": { - "textEnglish": "Technical Note: In Situ U\u2013Th\u2013He Dating By 4He\u2009\u2215\u20093He Laser Microprobe Analysis" + "esources": [ + { + "location": "https://gchron.copernicus.org/articles/5/323/2023/gchron-5-323-2023.pdf", + "source": "pub_pdf" + }, + { + "location": "https://gchron.copernicus.org/articles/5/323/2023/gchron-5-323-2023.html", + "source": "pub_html" + } + ], + "pagination": { + "electronicID": "18", + "firstPage": "323", + "lastPage": "332" }, - "abstract": { - "textEnglish": "In situ U\u2013Th\u2013He geochronology is a potentially disruptive technique that combines laser ablation inductively coupled plasma mass spectrometry (LA-ICP-MS) with laser microprobe noble gas mass spectrometry. Despite its potential to revolutionize (detrital) thermochronology, in situ U\u2013Th\u2013He dating is not widely used due to persistent analytical challenges. A major issue is that current in situ U\u2013Th\u2013He dating approaches require that the U, Th, and He measurements are expressed in units of molar concentration, in contrast with conventional methods, which use units of molar abundance. Whereas molar abundances can be reliably determined by isotope dilution, accurate concentration measurements are not so easy to obtain. In the absence of matrix-matched U\u2013Th concentration standards and accurate He ablation pit measurements, the required molar concentration calculations introduce an uncertainty that is higher than the conventional method, an uncertainty that is itself difficult to accurately quantify. We present a solution to this problem by using proton-induced 3He as a proxy for ablation pit volume and by pairing samples with a standard of known U\u2013Th\u2013He age. Thus, the U\u2013Th\u2013He age equation can be solved using relative rather than absolute concentration measurements. Pilot experiments show that the new method produces accurate results. However, it is prone to overdispersion, which is attributed to gradients in the proton fluence. These gradients can be measured, and their effect can be removed by fixing the geometry of the sample and the standard during the proton irradiation." + "persistentIDs": [ + { + "DOI": "10.5194/gchron-5-323-2023" + } + ], + "pubDate": { + "electrDate": "2023-07-19", + "printDate": "2023-07-19" + }, + "publication": { + "ISSN": [ + { + "issnString": "2628-3697", + "pubtype": "print" + }, + { + "issnString": "2628-3719", + "pubtype": "electronic" + } + ], + "pubName": "Geochronology", + "pubYear": "2023", + "volumeNum": "5" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ "Boyce, J. W., Hodges, K. V., Olszewski, W. J., Jercinovic, M. J., Carpenter, B. D., and Reiners, P. W.: Laser microprobe (U-Th)/He geochronology, Geochim. Cosmochim. Ac., 70, 3031\u20133039, https://doi.org/10.1016/j.gca.2006.03.019, 2006.\u2002a, b", @@ -135,14 +142,7 @@ "Vermeesch, P.: Logratio table of in-situ U-Th-4He/3He dated Fish Canyon zircon, Zenodo [data set], https://doi.org/10.5281/zenodo.8005223, 2023.\u2002a", "Vermeesch, P., Sherlock, S. C., Roberts, N. M. W., and Carter, A.: A simple method for in-situ U-Th-He dating, Geochim. Cosmochim. Ac., 79, 140\u2013147, https://doi.org/10.1016/j.gca.2011.11.042, 2012.\u2002a, b, c, d, e" ], - "esources": [ - { - "source": "pub_pdf", - "location": "https://gchron.copernicus.org/articles/5/323/2023/gchron-5-323-2023.pdf" - }, - { - "source": "pub_html", - "location": "https://gchron.copernicus.org/articles/5/323/2023/gchron-5-323-2023.html" - } - ] + "title": { + "textEnglish": "Technical Note: In Situ U\u2013Th\u2013He Dating By 4He\u2009\u2215\u20093He Laser Microprobe Analysis" + } } diff --git a/tests/stubdata/output/copernicus_ISPAn_isprs-annals-X-M-1-2023-237-2023.json b/tests/stubdata/output/copernicus_ISPAn_isprs-annals-X-M-1-2023-237-2023.json index ce1d52e..7bb8361 100644 --- a/tests/stubdata/output/copernicus_ISPAn_isprs-annals-X-M-1-2023-237-2023.json +++ b/tests/stubdata/output/copernicus_ISPAn_isprs-annals-X-M-1-2023-237-2023.json @@ -1,48 +1,9 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2023-06-23", - "printDate": "2023-06-23" - }, - "publication": { - "pubName": "ISPRS Annals of the Photogrammetry, Remote Sensing and Spatial Information Sciences", - "volumeNum": "X-M-1-2023", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "print", - "issnString": "2194-9042" - }, - { - "pubtype": "electronic", - "issnString": "2194-9050" - } - ] - }, - "pagination": { - "firstPage": "237", - "lastPage": "244" + "abstract": { + "textEnglish": "The article focuses on modern methods of mining activity documentation and visualization. The development of technologies that allow us to display 3D models are many in recent years, from web portals, augmented reality using smartphones or tablets to virtual reality glasses. These technologies give us a whole new way of looking at and viewing 3D models. In this study, we will use most of the available options to visualize mining activities in the UNESCO-protected Ore Mountains. Each of these technologies needs differently prepared data. Because each of these technologies have different limits, we need to find these limits and modify the 3D models. The ZEB Revo laser scanner was used for data acquisition, which uses SLAM technology and is much more suitable for such areas than conventional terrestrial scanners, with which the work is lengthy and not nearly as efficient, and not the least of which eliminates the time-consuming post-scan work of merging scans. Especially when using scanning for mining, where there is not quite enough to go around, manually splicing scans is a nightmare, and automatic post-production merging is also often problematic." }, - "persistentIDs": [ - { - "DOI": "10.5194/isprs-annals-X-M-1-2023-237-2023" - } - ], "authors": [ { - "name": { - "surname": "Pavelka", - "given_name": "K.", - "suffix": "jr.", - "pubraw": "K. Pavelka jr." - }, "affiliation": [ { "affPubRaw": "Czech Technical University in Prague, Faculty of Civil Engineering, 16629 Prague 6, Thakurova 7, Czech Republic" @@ -50,14 +11,15 @@ ], "attrib": { "email": "karel.pavelka@cvut.cz" + }, + "name": { + "given_name": "K.", + "pubraw": "K. Pavelka jr.", + "suffix": "jr.", + "surname": "Pavelka" } }, { - "name": { - "surname": "B\u011bloch", - "given_name": "L.", - "pubraw": "L. B\u011bloch" - }, "affiliation": [ { "affPubRaw": "Czech Technical University in Prague, Faculty of Civil Engineering, 16629 Prague 6, Thakurova 7, Czech Republic" @@ -65,14 +27,14 @@ ], "attrib": { "email": "lukas.beloch@fsv.cvut.cz" + }, + "name": { + "given_name": "L.", + "pubraw": "L. B\u011bloch", + "surname": "B\u011bloch" } }, { - "name": { - "surname": "Pavelka", - "given_name": "K.", - "pubraw": "K. Pavelka" - }, "affiliation": [ { "affPubRaw": "Czech Technical University in Prague, Faculty of Civil Engineering, 16629 Prague 6, Thakurova 7, Czech Republic" @@ -80,23 +42,61 @@ ], "attrib": { "email": "pavelka@fsv.cvut.cz" + }, + "name": { + "given_name": "K.", + "pubraw": "K. Pavelka", + "surname": "Pavelka" } } ], - "title": { - "textEnglish": "Modern Methods Of Documentation And Visualization Of Historical Mines In The Unesco Mining Region In The Ore Mountains" - }, - "abstract": { - "textEnglish": "The article focuses on modern methods of mining activity documentation and visualization. The development of technologies that allow us to display 3D models are many in recent years, from web portals, augmented reality using smartphones or tablets to virtual reality glasses. These technologies give us a whole new way of looking at and viewing 3D models. In this study, we will use most of the available options to visualize mining activities in the UNESCO-protected Ore Mountains. Each of these technologies needs differently prepared data. Because each of these technologies have different limits, we need to find these limits and modify the 3D models. The ZEB Revo laser scanner was used for data acquisition, which uses SLAM technology and is much more suitable for such areas than conventional terrestrial scanners, with which the work is lengthy and not nearly as efficient, and not the least of which eliminates the time-consuming post-scan work of merging scans. Especially when using scanning for mining, where there is not quite enough to go around, manually splicing scans is a nightmare, and automatic post-production merging is also often problematic." - }, "esources": [ { - "source": "pub_pdf", - "location": "https://isprs-annals.copernicus.org/articles/X-M-1-2023/237/2023/isprs-annals-X-M-1-2023-237-2023.pdf" + "location": "https://isprs-annals.copernicus.org/articles/X-M-1-2023/237/2023/isprs-annals-X-M-1-2023-237-2023.pdf", + "source": "pub_pdf" }, { - "source": "pub_html", - "location": "https://isprs-annals.copernicus.org/articles/X-M-1-2023/237/2023/isprs-annals-X-M-1-2023-237-2023.html" + "location": "https://isprs-annals.copernicus.org/articles/X-M-1-2023/237/2023/isprs-annals-X-M-1-2023-237-2023.html", + "source": "pub_html" } - ] + ], + "pagination": { + "firstPage": "237", + "lastPage": "244" + }, + "persistentIDs": [ + { + "DOI": "10.5194/isprs-annals-X-M-1-2023-237-2023" + } + ], + "pubDate": { + "electrDate": "2023-06-23", + "printDate": "2023-06-23" + }, + "publication": { + "ISSN": [ + { + "issnString": "2194-9042", + "pubtype": "print" + }, + { + "issnString": "2194-9050", + "pubtype": "electronic" + } + ], + "pubName": "ISPRS Annals of the Photogrammetry, Remote Sensing and Spatial Information Sciences", + "pubYear": "2023", + "volumeNum": "X-M-1-2023" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "title": { + "textEnglish": "Modern Methods Of Documentation And Visualization Of Historical Mines In The Unesco Mining Region In The Ore Mountains" + } } diff --git a/tests/stubdata/output/copernicus_ISPAr_isprs-archives-XLVIII-M-2-2023-721-2023.json b/tests/stubdata/output/copernicus_ISPAr_isprs-archives-XLVIII-M-2-2023-721-2023.json index b63aff0..b5ddaf3 100644 --- a/tests/stubdata/output/copernicus_ISPAr_isprs-archives-XLVIII-M-2-2023-721-2023.json +++ b/tests/stubdata/output/copernicus_ISPAr_isprs-archives-XLVIII-M-2-2023-721-2023.json @@ -1,47 +1,9 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2023-06-24", - "printDate": "2023-06-24" - }, - "publication": { - "pubName": "The International Archives of the Photogrammetry, Remote Sensing and Spatial Information Sciences", - "volumeNum": "XLVIII-M-2-2023", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "print", - "issnString": "1682-1750" - }, - { - "pubtype": "electronic", - "issnString": "2194-9034" - } - ] - }, - "pagination": { - "firstPage": "721", - "lastPage": "727" + "abstract": { + "textEnglish": "3D imaging of large painted and vaulted historic ceilings offers many challenges, including those due to complex small and large-scale geometry, environmental conditions and limited access. In this paper we introduce CHAPI (Cultural Heritage Automated Photogrammetric Imaging), a low cost solution to these problems which provides an efficient, semi-automated method of capturing large vaulted ceiling paintings in high detail, with a consistent photogrammetric network and in limited time. We will present and examine two different case studies from the Plafond3D project, the baroque ceiling paintings of the Schloss Rheinsberg Spiegelsaal (mirror room) and the Ansbach Residence Festsaal (great hall/ballroom). The paper will examine the particular challenges of capturing large painted areas with accurate colour and geometric reproduction, and suggest how the photogrammetric recording and reconstruction process of ceilings can be optimised for large rooms. This paper also gives technical specifications and Open Access Code for the CHAPI build." }, - "persistentIDs": [ - { - "DOI": "10.5194/isprs-archives-XLVIII-M-2-2023-721-2023" - } - ], "authors": [ { - "name": { - "surname": "Hindmarch", - "given_name": "J.", - "pubraw": "J. Hindmarch" - }, "affiliation": [ { "affPubRaw": "Digital Technologies in Heritage Conservation, Institute of Archaeology, Heritage Conservation Studies and Art History, University of Bamberg, 96047, Germany" @@ -49,14 +11,14 @@ ], "attrib": { "email": "johnhindmarch@gmail.com" + }, + "name": { + "given_name": "J.", + "pubraw": "J. Hindmarch", + "surname": "Hindmarch" } }, { - "name": { - "surname": "Hess", - "given_name": "M.", - "pubraw": "M. Hess" - }, "affiliation": [ { "affPubRaw": "Digital Technologies in Heritage Conservation, Institute of Archaeology, Heritage Conservation Studies and Art History, University of Bamberg, 96047, Germany" @@ -64,14 +26,14 @@ ], "attrib": { "email": "mona.hess@uni-bamberg.de" + }, + "name": { + "given_name": "M.", + "pubraw": "M. Hess", + "surname": "Hess" } }, { - "name": { - "surname": "Groh", - "given_name": "M.", - "pubraw": "M. Groh" - }, "affiliation": [ { "affPubRaw": "Digital Technologies in Heritage Conservation, Institute of Archaeology, Heritage Conservation Studies and Art History, University of Bamberg, 96047, Germany" @@ -79,14 +41,14 @@ ], "attrib": { "email": "michael.groh@uni-bamberg.de" + }, + "name": { + "given_name": "M.", + "pubraw": "M. Groh", + "surname": "Groh" } }, { - "name": { - "surname": "Burioni", - "given_name": "M.", - "pubraw": "M. Burioni" - }, "affiliation": [ { "affPubRaw": "Corpus of Baroque Ceiling Paintings, Institute of Art History, LMU Munich, 80798, Germany" @@ -94,23 +56,61 @@ ], "attrib": { "email": "matteo.burioni@lmu.de" + }, + "name": { + "given_name": "M.", + "pubraw": "M. Burioni", + "surname": "Burioni" } } ], - "title": { - "textEnglish": "A Semi-Automated Methodology For 3D Imaging Of Large Vaulted Ceiling Paintings" - }, - "abstract": { - "textEnglish": "3D imaging of large painted and vaulted historic ceilings offers many challenges, including those due to complex small and large-scale geometry, environmental conditions and limited access. In this paper we introduce CHAPI (Cultural Heritage Automated Photogrammetric Imaging), a low cost solution to these problems which provides an efficient, semi-automated method of capturing large vaulted ceiling paintings in high detail, with a consistent photogrammetric network and in limited time. We will present and examine two different case studies from the Plafond3D project, the baroque ceiling paintings of the Schloss Rheinsberg Spiegelsaal (mirror room) and the Ansbach Residence Festsaal (great hall/ballroom). The paper will examine the particular challenges of capturing large painted areas with accurate colour and geometric reproduction, and suggest how the photogrammetric recording and reconstruction process of ceilings can be optimised for large rooms. This paper also gives technical specifications and Open Access Code for the CHAPI build." - }, "esources": [ { - "source": "pub_pdf", - "location": "https://isprs-archives.copernicus.org/articles/XLVIII-M-2-2023/721/2023/isprs-archives-XLVIII-M-2-2023-721-2023.pdf" + "location": "https://isprs-archives.copernicus.org/articles/XLVIII-M-2-2023/721/2023/isprs-archives-XLVIII-M-2-2023-721-2023.pdf", + "source": "pub_pdf" }, { - "source": "pub_html", - "location": "https://isprs-archives.copernicus.org/articles/XLVIII-M-2-2023/721/2023/isprs-archives-XLVIII-M-2-2023-721-2023.html" + "location": "https://isprs-archives.copernicus.org/articles/XLVIII-M-2-2023/721/2023/isprs-archives-XLVIII-M-2-2023-721-2023.html", + "source": "pub_html" + } + ], + "pagination": { + "firstPage": "721", + "lastPage": "727" + }, + "persistentIDs": [ + { + "DOI": "10.5194/isprs-archives-XLVIII-M-2-2023-721-2023" } - ] + ], + "pubDate": { + "electrDate": "2023-06-24", + "printDate": "2023-06-24" + }, + "publication": { + "ISSN": [ + { + "issnString": "1682-1750", + "pubtype": "print" + }, + { + "issnString": "2194-9034", + "pubtype": "electronic" + } + ], + "pubName": "The International Archives of the Photogrammetry, Remote Sensing and Spatial Information Sciences", + "pubYear": "2023", + "volumeNum": "XLVIII-M-2-2023" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "title": { + "textEnglish": "A Semi-Automated Methodology For 3D Imaging Of Large Vaulted Ceiling Paintings" + } } diff --git a/tests/stubdata/output/crossref_10.1002_1521-3994.json b/tests/stubdata/output/crossref_10.1002_1521-3994.json index a840cba..c94939b 100644 --- a/tests/stubdata/output/crossref_10.1002_1521-3994.json +++ b/tests/stubdata/output/crossref_10.1002_1521-3994.json @@ -1,50 +1,53 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "printDate": "1999-03-00" - }, - "publication": { - "pubName": "Astronomische Nachrichten", - "issueNum": "1", - "volumeNum": "320", - "pubYear": "1999", - "ISSN": [ - { - "pubtype": "print", - "issnString": "0004-6337" - }, - { - "pubtype": "electronic", - "issnString": "1521-3994" + "authors": [ + { + "name": { + "given_name": "E.", + "surname": "Schmutzer" } - ] - }, - "persistentIDs": [ + } + ], + "esources": [ { - "DOI": "10.1002/1521-3994(199903)320:1<1::AID-ASNA1>3.0.CO;2-8" + "location": "https://onlinelibrary.wiley.com/doi/10.1002/1521-3994(199903)320:1<1::AID-ASNA1>3.0.CO;2-8", + "source": "pub_html" } ], "pagination": { "firstPage": "1", "lastPage": "19" }, - "authors": [ + "persistentIDs": [ { - "name": { - "surname": "Schmutzer", - "given_name": "E." - } + "DOI": "10.1002/1521-3994(199903)320:1<1::AID-ASNA1>3.0.CO;2-8" } ], - "title": { - "textEnglish": "Cosmology without Big Bang within the framework of the Projective Unified Field Theory and the influence on the motion of cosmic objects" + "pubDate": { + "printDate": "1999-03-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "0004-6337", + "pubtype": "print" + }, + { + "issnString": "1521-3994", + "pubtype": "electronic" + } + ], + "issueNum": "1", + "pubName": "Astronomische Nachrichten", + "pubYear": "1999", + "volumeNum": "320" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ "3.0.CO;2-8-BIB1\"> Astron. Nachr. Avakian 311 343 1990 10.1002/asna.2113110604 ", @@ -64,10 +67,7 @@ "3.0.CO;2-8-BIB15\"> Schmutzer 1998 : 1998, Schriften der Sudetendeutschen Akademie der Wissenschaften und K\u00fcnste in M\u00fcnchen, 19, p. 153; Abstract in: P. Brosche et al. (eds.): \u201cThe Message of the Angles - Astronomy from 1798 to 1998\u201d, H. Deutsch 1998, p. 259 (Conf. Astronomische Gesellschaft, Gotha, May 1998 ", "3.0.CO;2-8-BIB16\"> Zimmermann and : ABC-Lexikon Astronomie. 8th Edition, Spektrum Address of the author: Ernst Schmutzer Cospedaer Grund 57 " ], - "esources": [ - { - "source": "pub_html", - "location": "https://onlinelibrary.wiley.com/doi/10.1002/1521-3994(199903)320:1<1::AID-ASNA1>3.0.CO;2-8" - } - ] + "title": { + "textEnglish": "Cosmology without Big Bang within the framework of the Projective Unified Field Theory and the influence on the motion of cosmic objects" + } } diff --git a/tests/stubdata/output/crossref_10.1103_PhysRevD_64-117303.json b/tests/stubdata/output/crossref_10.1103_PhysRevD_64-117303.json index 32ecea8..68677c9 100644 --- a/tests/stubdata/output/crossref_10.1103_PhysRevD_64-117303.json +++ b/tests/stubdata/output/crossref_10.1103_PhysRevD_64-117303.json @@ -1,55 +1,58 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" + "authors": [ + { + "name": { + "given_name": "Ernest", + "surname": "Ma" + } + }, + { + "name": { + "given_name": "G.", + "surname": "Rajasekaran" + } + } + ], + "esources": [ + { + "location": "https://link.aps.org/doi/10.1103/PhysRevD.64.117303", + "source": "pub_html" + } + ], + "pagination": { + "electronicID": "117303" }, + "persistentIDs": [ + { + "DOI": "10.1103/PhysRevD.64.117303" + } + ], "pubDate": { "electrDate": "2001-11-08" }, "publication": { - "pubName": "Physical Review D", - "issueNum": "11", - "volumeNum": "64", - "pubYear": "2001", "ISSN": [ { - "pubtype": "print", - "issnString": "0556-2821" + "issnString": "0556-2821", + "pubtype": "print" }, { - "pubtype": "electronic", - "issnString": "1089-4918" + "issnString": "1089-4918", + "pubtype": "electronic" } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1103/PhysRevD.64.117303" - } - ], - "pagination": { - "electronicID": "117303" + ], + "issueNum": "11", + "pubName": "Physical Review D", + "pubYear": "2001", + "volumeNum": "64" }, - "authors": [ - { - "name": { - "surname": "Ma", - "given_name": "Ernest" - } - }, - { - "name": { - "surname": "Rajasekaran", - "given_name": "G." - } - } - ], - "title": { - "textEnglish": "Light unstable sterile neutrino" + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " Phys. Rev. Lett. S. Fukuda 85 3999 2000 10.1103/PhysRevLett.85.3999 ", @@ -79,10 +82,7 @@ " Nucl. Phys. K.A. Olive B180 497 1981 10.1016/0550-3213(81)90065-1 ", " Phys. Lett. J. Ellis 167B 457 1986 10.1016/0370-2693(86)91301-8 " ], - "esources": [ - { - "source": "pub_html", - "location": "https://link.aps.org/doi/10.1103/PhysRevD.64.117303" - } - ] + "title": { + "textEnglish": "Light unstable sterile neutrino" + } } diff --git a/tests/stubdata/output/crossref_10.1146_annurev.energy.25.1.441.json b/tests/stubdata/output/crossref_10.1146_annurev.energy.25.1.441.json index 67833f1..4afd536 100644 --- a/tests/stubdata/output/crossref_10.1146_annurev.energy.25.1.441.json +++ b/tests/stubdata/output/crossref_10.1146_annurev.energy.25.1.441.json @@ -1,65 +1,68 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "printDate": "2000-11-00" - }, - "publication": { - "pubName": "Annual Review of Energy and the Environment", - "issueNum": "1", - "volumeNum": "25", - "pubYear": "2000", - "ISSN": [ - { - "pubtype": "print", - "issnString": "1056-3466" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1146/annurev.energy.25.1.441" - } - ], - "pagination": { - "firstPage": "441", - "lastPage": "475" + "abstract": { + "textEnglish": "\u25aa Abstract Water vapor is the dominant greenhouse gas, the most important gaseous source of infrared opacity in the atmosphere. As the concentrations of other greenhouse gases, particularly carbon dioxide, increase because of human activity, it is centrally important to predict how the water vapor distribution will be affected. To the extent that water vapor concentrations increase in a warmer world, the climatic effects of the other greenhouse gases will be amplified. Models of the Earth's climate indicate that this is an important positive feedback that increases the sensitivity of surface temperatures to carbon dioxide by nearly a factor of two when considered in isolation from other feedbacks, and possibly by as much as a factor of three or more when interactions with other feedbacks are considered. Critics of this consensus have attempted to provide reasons why modeling results are overestimating the strength of this feedback. Our uncertainty concerning climate sensitivity is disturbing. The range most often quoted for the equilibrium global mean surface temperature response to a doubling of CO 2 concentrations in the atmosphere is 1.5\u00b0C to 4.5\u00b0C. If the Earth lies near the upper bound of this sensitivity range, climate changes in the twenty-first century will be profound. The range in sensitivity is primarily due to differing assumptions about how the Earth's cloud distribution is maintained; all the models on which these estimates are based possess strong water vapor feedback. If this feedback is, in fact, substantially weaker than predicted in current models, sensitivities in the upper half of this range would be much less likely, a conclusion that would clearly have important policy implications. In this review, we describe the background behind the prevailing view on water vapor feedback and some of the arguments raised by its critics, and attempt to explain why these arguments have not modified the consensus within the climate research community." }, "authors": [ { - "name": { - "surname": "Held", - "given_name": "Isaac M." - }, "affiliation": [ { "affPubRaw": "Geophysical Fluid Dynamics Laboratory/National Oceanic and Atmospheric Administration, Princeton, New Jersey 08542" } - ] + ], + "name": { + "given_name": "Isaac M.", + "surname": "Held" + } }, { - "name": { - "surname": "Soden", - "given_name": "Brian J." - }, "affiliation": [ { "affPubRaw": "Geophysical Fluid Dynamics Laboratory/National Oceanic and Atmospheric Administration, Princeton, New Jersey 08542" } - ] + ], + "name": { + "given_name": "Brian J.", + "surname": "Soden" + } } ], - "title": { - "textEnglish": "Water Vapor Feedback and Global Warming" + "esources": [ + { + "location": "https://www.annualreviews.org/doi/10.1146/annurev.energy.25.1.441", + "source": "pub_html" + } + ], + "pagination": { + "firstPage": "441", + "lastPage": "475" }, - "abstract": { - "textEnglish": "\u25aa Abstract Water vapor is the dominant greenhouse gas, the most important gaseous source of infrared opacity in the atmosphere. As the concentrations of other greenhouse gases, particularly carbon dioxide, increase because of human activity, it is centrally important to predict how the water vapor distribution will be affected. To the extent that water vapor concentrations increase in a warmer world, the climatic effects of the other greenhouse gases will be amplified. Models of the Earth's climate indicate that this is an important positive feedback that increases the sensitivity of surface temperatures to carbon dioxide by nearly a factor of two when considered in isolation from other feedbacks, and possibly by as much as a factor of three or more when interactions with other feedbacks are considered. Critics of this consensus have attempted to provide reasons why modeling results are overestimating the strength of this feedback. Our uncertainty concerning climate sensitivity is disturbing. The range most often quoted for the equilibrium global mean surface temperature response to a doubling of CO 2 concentrations in the atmosphere is 1.5\u00b0C to 4.5\u00b0C. If the Earth lies near the upper bound of this sensitivity range, climate changes in the twenty-first century will be profound. The range in sensitivity is primarily due to differing assumptions about how the Earth's cloud distribution is maintained; all the models on which these estimates are based possess strong water vapor feedback. If this feedback is, in fact, substantially weaker than predicted in current models, sensitivities in the upper half of this range would be much less likely, a conclusion that would clearly have important policy implications. In this review, we describe the background behind the prevailing view on water vapor feedback and some of the arguments raised by its critics, and attempt to explain why these arguments have not modified the consensus within the climate research community." + "persistentIDs": [ + { + "DOI": "10.1146/annurev.energy.25.1.441" + } + ], + "pubDate": { + "printDate": "2000-11-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "1056-3466", + "pubtype": "print" + } + ], + "issueNum": "1", + "pubName": "Annual Review of Energy and the Environment", + "pubYear": "2000", + "volumeNum": "25" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " Fourier JB. 1827. Memoire sur les temperatures du globe terrestre et des espaces planetaires. Mem. Acad. R. Sci. Inst. France7:569\u2013604 ", @@ -152,10 +155,7 @@ " 10.1029/1998GL900169 ", " 10.1175/1520-0442(2000)013<3337:DVITWV>2.0.CO;2 " ], - "esources": [ - { - "source": "pub_html", - "location": "https://www.annualreviews.org/doi/10.1146/annurev.energy.25.1.441" - } - ] + "title": { + "textEnglish": "Water Vapor Feedback and Global Warming" + } } diff --git a/tests/stubdata/output/crossref_10.3137_a0410105.json b/tests/stubdata/output/crossref_10.3137_a0410105.json index d9ded0a..7ddd36d 100644 --- a/tests/stubdata/output/crossref_10.3137_a0410105.json +++ b/tests/stubdata/output/crossref_10.3137_a0410105.json @@ -1,68 +1,71 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "printDate": "2003-03-00" - }, - "publication": { - "pubName": "Atmosphere-Ocean", - "issueNum": "1", - "volumeNum": "41", - "pubYear": "2003", - "ISSN": [ - { - "pubtype": "print", - "issnString": "0705-5900" - }, - { - "pubtype": "electronic", - "issnString": "1480-9214" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.3137/ao.410105" - } - ], - "pagination": { - "firstPage": "65", - "lastPage": "98" - }, "authors": [ { "name": { - "surname": "Article", - "given_name": "Survey" + "given_name": "Survey", + "surname": "Article" } }, { "name": { - "surname": "Kim", - "given_name": "Young\u2010Joon" + "given_name": "Young\u2010Joon", + "surname": "Kim" } }, { "name": { - "surname": "Eckermann", - "given_name": "Stephen D." + "given_name": "Stephen D.", + "surname": "Eckermann" } }, { "name": { - "surname": "Chun", - "given_name": "Hye\u2010Yeong" + "given_name": "Hye\u2010Yeong", + "surname": "Chun" } } ], - "title": { - "textEnglish": "An overview of the past, present and future of gravity\u2010wave drag parametrization for numerical climate and weather prediction models" + "esources": [ + { + "location": "http://www.tandfonline.com/doi/abs/10.3137/ao.410105", + "source": "pub_html" + } + ], + "pagination": { + "firstPage": "65", + "lastPage": "98" + }, + "persistentIDs": [ + { + "DOI": "10.3137/ao.410105" + } + ], + "pubDate": { + "printDate": "2003-03-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "0705-5900", + "pubtype": "print" + }, + { + "issnString": "1480-9214", + "pubtype": "electronic" + } + ], + "issueNum": "1", + "pubName": "Atmosphere-Ocean", + "pubYear": "2003", + "volumeNum": "41" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " 10.1029/2000JD900520 ", @@ -369,10 +372,7 @@ " 10.1002/qj.49712757702 ", " 10.1002/qj.49712253206 " ], - "esources": [ - { - "source": "pub_html", - "location": "http://www.tandfonline.com/doi/abs/10.3137/ao.410105" - } - ] + "title": { + "textEnglish": "An overview of the past, present and future of gravity\u2010wave drag parametrization for numerical climate and weather prediction models" + } } diff --git a/tests/stubdata/output/crossref_10.3847_2041-8213.json b/tests/stubdata/output/crossref_10.3847_2041-8213.json index a2463d3..af09c06 100644 --- a/tests/stubdata/output/crossref_10.3847_2041-8213.json +++ b/tests/stubdata/output/crossref_10.3847_2041-8213.json @@ -1,86 +1,93 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2020-11-09" - ], - "acceptedDate": "2020-12-09" - }, - "pubDate": { - "electrDate": "2021-01-13", - "printDate": "2021-01-01" - }, - "publication": { - "pubName": "The Astrophysical Journal Letters", - "issueNum": "2", - "volumeNum": "906", - "pubYear": "2021", - "ISSN": [ - { - "pubtype": "print", - "issnString": "2041-8205" - }, - { - "pubtype": "electronic", - "issnString": "2041-8213" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.3847/2041-8213/abd256" - } - ], - "pagination": { - "firstPage": "L14" + "abstract": { + "textEnglish": "We present the results of a search in LIGO O2 public data for continuous gravitational waves from the neutron star in the low-mass X-ray binary Scorpius X-1. We search for signals with \u2248 constant frequency in the range 40\u2013180 Hz. Thanks to the efficiency of our search pipeline we can use a long coherence time and achieve unprecedented sensitivity, significantly improving on existing results. This is the first search that has been able to probe gravitational wave amplitudes that could balance the accretion torque at the neutron star radius. Our search excludes emission at this level between 67.5 and 131.5 Hz, for an inclination angle 44\u00b0 \u00b1 6\u00b0 derived from radio observations, and assuming that the spin axis is perpendicular to the orbital plane. If the torque arm is \u224826 km\u2014a conservative estimate of the Alfv\u00e9n radius\u2014our results are more constraining than the indirect limit across the band. This allows us to exclude certain mass\u2013radius combinations and to place upper limits on the strength of the star\u2019s magnetic field with a different probe than ever used before. We also correct a mistake that appears in the literature in the equation that gives the gravitational wave amplitude at the torque balance and we re-interpret the associated latest LIGO/Virgo results in light of this." }, "authors": [ { "name": { - "surname": "Zhang", - "given_name": "Yuanhao" + "given_name": "Yuanhao", + "surname": "Zhang" } }, { - "name": { - "surname": "Papa", - "given_name": "Maria Alessandra" - }, "attrib": { "orcid": "0000-0002-1007-5298" + }, + "name": { + "given_name": "Maria Alessandra", + "surname": "Papa" } }, { - "name": { - "surname": "Krishnan", - "given_name": "Badri" - }, "attrib": { "orcid": "0000-0003-3015-234X" + }, + "name": { + "given_name": "Badri", + "surname": "Krishnan" } }, { - "name": { - "surname": "Watts", - "given_name": "Anna L." - }, "attrib": { "orcid": "0000-0002-1009-2354" + }, + "name": { + "given_name": "Anna L.", + "surname": "Watts" } } ], - "title": { - "textEnglish": "Search for Continuous Gravitational Waves from Scorpius X-1 in LIGO O2 Data" + "copyright": { + "statement": "\u00a9 2021. The Author(s). Published by the American Astronomical Society.", + "status": true }, - "abstract": { - "textEnglish": "We present the results of a search in LIGO O2 public data for continuous gravitational waves from the neutron star in the low-mass X-ray binary Scorpius X-1. We search for signals with \u2248 constant frequency in the range 40\u2013180 Hz. Thanks to the efficiency of our search pipeline we can use a long coherence time and achieve unprecedented sensitivity, significantly improving on existing results. This is the first search that has been able to probe gravitational wave amplitudes that could balance the accretion torque at the neutron star radius. Our search excludes emission at this level between 67.5 and 131.5 Hz, for an inclination angle 44\u00b0 \u00b1 6\u00b0 derived from radio observations, and assuming that the spin axis is perpendicular to the orbital plane. If the torque arm is \u224826 km\u2014a conservative estimate of the Alfv\u00e9n radius\u2014our results are more constraining than the indirect limit across the band. This allows us to exclude certain mass\u2013radius combinations and to place upper limits on the strength of the star\u2019s magnetic field with a different probe than ever used before. We also correct a mistake that appears in the literature in the equation that gives the gravitational wave amplitude at the torque balance and we re-interpret the associated latest LIGO/Virgo results in light of this." + "editorialHistory": { + "acceptedDate": "2020-12-09", + "receivedDates": [ + "2020-11-09" + ] + }, + "esources": [ + { + "location": "https://iopscience.iop.org/article/10.3847/2041-8213/abd256", + "source": "pub_html" + } + ], + "pagination": { + "firstPage": "L14" + }, + "persistentIDs": [ + { + "DOI": "10.3847/2041-8213/abd256" + } + ], + "pubDate": { + "electrDate": "2021-01-13", + "printDate": "2021-01-01" + }, + "publication": { + "ISSN": [ + { + "issnString": "2041-8205", + "pubtype": "print" + }, + { + "issnString": "2041-8213", + "pubtype": "electronic" + } + ], + "issueNum": "2", + "pubName": "The Astrophysical Journal Letters", + "pubYear": "2021", + "volumeNum": "906" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " PhRvD Abbott 10.1103/PhysRevD.100.122002 100 122002 2019a ", @@ -153,14 +160,7 @@ " ApJL Woan 10.3847/2041-8213/aad86a 863 L40 2018 ", " Zhang 2020 " ], - "esources": [ - { - "source": "pub_html", - "location": "https://iopscience.iop.org/article/10.3847/2041-8213/abd256" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 2021. The Author(s). Published by the American Astronomical Society." + "title": { + "textEnglish": "Search for Continuous Gravitational Waves from Scorpius X-1 in LIGO O2 Data" } } diff --git a/tests/stubdata/output/crossref_book_10.1007-978-1-4614-3520-4.json b/tests/stubdata/output/crossref_book_10.1007-978-1-4614-3520-4.json index 2ca50be..6772f4c 100644 --- a/tests/stubdata/output/crossref_book_10.1007-978-1-4614-3520-4.json +++ b/tests/stubdata/output/crossref_book_10.1007-978-1-4614-3520-4.json @@ -1,67 +1,67 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "printDate": "2012-00-00" - }, - "publication": { - "publisher": "Springer New York", - "volumeNum": "902", - "pubYear": "2012", - "bookSeries": { - "seriesName": "Lecture Notes in Statistics", - "seriesID": "0930-0325", - "seriesDescription": "issn" - } - }, - "persistentIDs": [ + "esources": [ { - "ISBN": [ - { - "pubtype": "print", - "isbnString": "978-1-4614-3519-8" - }, - { - "pubtype": "electronic", - "isbnString": "978-1-4614-3520-4" - } - ], - "DOI": "10.1007/978-1-4614-3520-4" + "location": "http://link.springer.com/10.1007/978-1-4614-3520-4", + "source": "pub_html" } ], "otherContributor": [ { - "role": "editor", "contrib": { "name": { - "surname": "Feigelson", - "given_name": "Eric D." + "given_name": "Eric D.", + "surname": "Feigelson" } - } + }, + "role": "editor" }, { - "role": "editor", "contrib": { "name": { - "surname": "Babu", - "given_name": "G. Jogesh" + "given_name": "G. Jogesh", + "surname": "Babu" } - } + }, + "role": "editor" } ], - "title": { - "textEnglish": "Lecture Notes in Statistics" - }, - "esources": [ + "persistentIDs": [ { - "source": "pub_html", - "location": "http://link.springer.com/10.1007/978-1-4614-3520-4" + "DOI": "10.1007/978-1-4614-3520-4", + "ISBN": [ + { + "isbnString": "978-1-4614-3519-8", + "pubtype": "print" + }, + { + "isbnString": "978-1-4614-3520-4", + "pubtype": "electronic" + } + ] } - ] + ], + "pubDate": { + "printDate": "2012-00-00" + }, + "publication": { + "bookSeries": { + "seriesDescription": "issn", + "seriesID": "0930-0325", + "seriesName": "Lecture Notes in Statistics" + }, + "pubYear": "2012", + "publisher": "Springer New York", + "volumeNum": "902" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "title": { + "textEnglish": "Lecture Notes in Statistics" + } } diff --git a/tests/stubdata/output/crossref_book_10.1017-CBO9780511709265.json b/tests/stubdata/output/crossref_book_10.1017-CBO9780511709265.json index f8d6b33..ecc49d1 100644 --- a/tests/stubdata/output/crossref_book_10.1017-CBO9780511709265.json +++ b/tests/stubdata/output/crossref_book_10.1017-CBO9780511709265.json @@ -1,46 +1,46 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2009-00-00", - "printDate": "2010-00-00" - }, - "publication": { - "publisher": "Cambridge University Press", - "pubYear": "2010" - }, - "persistentIDs": [ - { - "ISBN": [ - { - "pubtype": "print", - "isbnString": "9780511709265" - } - ], - "DOI": "10.1017/CBO9780511709265" - } - ], "authors": [ { "name": { - "surname": "Clerke", - "given_name": "Agnes Mary" + "given_name": "Agnes Mary", + "surname": "Clerke" } } ], - "title": { - "textEnglish": "The Herschels and Modern Astronomy" - }, "esources": [ { - "source": "pub_html", - "location": "http://ebooks.cambridge.org/ref/id/CBO9780511709265" + "location": "http://ebooks.cambridge.org/ref/id/CBO9780511709265", + "source": "pub_html" } - ] + ], + "persistentIDs": [ + { + "DOI": "10.1017/CBO9780511709265", + "ISBN": [ + { + "isbnString": "9780511709265", + "pubtype": "print" + } + ] + } + ], + "pubDate": { + "electrDate": "2009-00-00", + "printDate": "2010-00-00" + }, + "publication": { + "pubYear": "2010", + "publisher": "Cambridge University Press" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "title": { + "textEnglish": "The Herschels and Modern Astronomy" + } } diff --git a/tests/stubdata/output/crossref_cn_10.1051=0004-6361=202243540.json b/tests/stubdata/output/crossref_cn_10.1051=0004-6361=202243540.json index 8f49b39..572d543 100644 --- a/tests/stubdata/output/crossref_cn_10.1051=0004-6361=202243540.json +++ b/tests/stubdata/output/crossref_cn_10.1051=0004-6361=202243540.json @@ -1,79 +1,79 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2022-11-09", - "printDate": "2022-11-00" - }, - "publication": { - "pubName": "Astronomy & Astrophysics", - "volumeNum": "667", - "pubYear": "2022", - "ISSN": [ - { - "pubtype": "print", - "issnString": "0004-6361" - }, - { - "pubtype": "electronic", - "issnString": "1432-0746" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1051/0004-6361/202243540" - } - ], - "pagination": { - "firstPage": "A75" + "abstract": { + "textEnglish": "Aims. We present the implementation of the treatment of particle ejection and dust nucleation in the smoothed particle hydrodynamics (SPH) code P HANTOM . These developments represent the first step toward a more complete modeling of dust-driven winds emanating from asymptotic giant branch (AGB) stars that can be used for comparison with high resolution imaging of these stars. Methods. The AGB outflow is modeled by injecting the SPH particles from a spherical inner boundary. This boundary is a series of concentric shells, with the AGB star at its center, and the particles are positioned on these shells on the vertices of an isocahedron geodesic surface. The outermost shell is ejected with a predefined radial velocity, and subsequent lower shells replenish the ejected ones, all rotated randomly to improve the isotropy of the outflow. The physical properties of the particles on these shells are set by solving the 1D analytic steady wind equations. The formation of dust is calculated starting from a compact chemical network for carbon-rich material, which creates the building blocks of the solid-state particles. Subsequently, the theory of the moments is used to obtain dust growth rates, without requiring knowledge on the grain size distribution. Results. We tested our implementation against a series of 1D reference solutions. We demonstrate that our method is able to reproduce Parker-type wind solutions. For the trans-sonic solution, small oscillations are present in the vicinity of the sonic point, but these do not impact the trans-sonic passage or terminal wind velocity. Supersonic solutions always compare nicely with 1D analytic profiles. We also tested our implementation of dust using two formalisms: an analytic prescription for the opacity devised by Bowen and the full treatment of carbon-dust formation. Both simulations reproduce the 1D analytic solution displaying the expected additional acceleration when the gas temperature falls below the condensation temperature." }, "authors": [ { - "name": { - "surname": "Siess", - "given_name": "L." - }, "attrib": { "orcid": "0000-0001-6008-1103" + }, + "name": { + "given_name": "L.", + "surname": "Siess" } }, { "name": { - "surname": "Homan", - "given_name": "W." + "given_name": "W.", + "surname": "Homan" } }, { "name": { - "surname": "Toupin", - "given_name": "S." + "given_name": "S.", + "surname": "Toupin" } }, { - "name": { - "surname": "Price", - "given_name": "D. J." - }, "attrib": { "orcid": "0000-0002-4716-4235" + }, + "name": { + "given_name": "D. J.", + "surname": "Price" } } ], - "title": { - "textEnglish": "3D simulations of AGB stellar winds" + "esources": [ + { + "location": "https://www.aanda.org/10.1051/0004-6361/202243540", + "source": "pub_html" + } + ], + "pagination": { + "firstPage": "A75" }, - "subtitle": { - "textEnglish": "I. Steady winds and dust formation" + "persistentIDs": [ + { + "DOI": "10.1051/0004-6361/202243540" + } + ], + "pubDate": { + "electrDate": "2022-11-09", + "printDate": "2022-11-00" }, - "abstract": { - "textEnglish": "Aims. We present the implementation of the treatment of particle ejection and dust nucleation in the smoothed particle hydrodynamics (SPH) code P HANTOM . These developments represent the first step toward a more complete modeling of dust-driven winds emanating from asymptotic giant branch (AGB) stars that can be used for comparison with high resolution imaging of these stars. Methods. The AGB outflow is modeled by injecting the SPH particles from a spherical inner boundary. This boundary is a series of concentric shells, with the AGB star at its center, and the particles are positioned on these shells on the vertices of an isocahedron geodesic surface. The outermost shell is ejected with a predefined radial velocity, and subsequent lower shells replenish the ejected ones, all rotated randomly to improve the isotropy of the outflow. The physical properties of the particles on these shells are set by solving the 1D analytic steady wind equations. The formation of dust is calculated starting from a compact chemical network for carbon-rich material, which creates the building blocks of the solid-state particles. Subsequently, the theory of the moments is used to obtain dust growth rates, without requiring knowledge on the grain size distribution. Results. We tested our implementation against a series of 1D reference solutions. We demonstrate that our method is able to reproduce Parker-type wind solutions. For the trans-sonic solution, small oscillations are present in the vicinity of the sonic point, but these do not impact the trans-sonic passage or terminal wind velocity. Supersonic solutions always compare nicely with 1D analytic profiles. We also tested our implementation of dust using two formalisms: an analytic prescription for the opacity devised by Bowen and the full treatment of carbon-dust formation. Both simulations reproduce the 1D analytic solution displaying the expected additional acceleration when the gas temperature falls below the condensation temperature." + "publication": { + "ISSN": [ + { + "issnString": "0004-6361", + "pubtype": "print" + }, + { + "issnString": "1432-0746", + "pubtype": "electronic" + } + ], + "pubName": "Astronomy & Astrophysics", + "pubYear": "2022", + "volumeNum": "667" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " MNRAS Altay 434 748 2013 10.1093/mnras/stt1067 ", @@ -178,10 +178,10 @@ " MNRAS Whitehouse 364 1367 2005 10.1111/j.1365-2966.2005.09683.x ", " A&A Winters 361 641 2000 " ], - "esources": [ - { - "source": "pub_html", - "location": "https://www.aanda.org/10.1051/0004-6361/202243540" - } - ] + "subtitle": { + "textEnglish": "I. Steady winds and dust formation" + }, + "title": { + "textEnglish": "3D simulations of AGB stellar winds" + } } diff --git a/tests/stubdata/output/crossref_cn_10.1088=1475-7516=2022=10=098.json b/tests/stubdata/output/crossref_cn_10.1088=1475-7516=2022=10=098.json index 06f838e..28e8e0d 100644 --- a/tests/stubdata/output/crossref_cn_10.1088=1475-7516=2022=10=098.json +++ b/tests/stubdata/output/crossref_cn_10.1088=1475-7516=2022=10=098.json @@ -1,67 +1,74 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2022-05-06" - ], - "acceptedDate": "2022-10-16" - }, - "pubDate": { - "electrDate": "2022-10-31", - "printDate": "2022-10-01" - }, - "publication": { - "pubName": "Journal of Cosmology and Astroparticle Physics", - "issueNum": "10", - "volumeNum": "2022", - "pubYear": "2022", - "ISSN": [ - { - "pubtype": "electronic", - "issnString": "1475-7516" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1088/1475-7516/2022/10/098" - } - ], - "pagination": { - "firstPage": "098" + "abstract": { + "textEnglish": "Microlensing of extragalactic sources, in particular the probability of significant amplifications, is a potentially powerful probe of the abundance of compact objects outside the halo of the Milky Way. Accurate experimental constraints require an equally accurate theoretical model for the amplification statistics produced by such a population. In this article, we argue that the simplest (strongest-lens) model does not meet this demanding requirement. We thus propose an elaborate practical modelling scheme for extragalactic microlensing. We derive from first principles an expression for the amplification probability that consistently allows for: (i) the coupling between microlenses; (ii) realistic perturbations from the cosmic large-scale structure; (iii) extended-source corrections. An important conclusion is that the external shear applied on the dominant microlens, both by the other lenses and by the large-scale structure, is practically negligible. Yet, the predictions of our approach can still differ by a factor of a few with respect to existing models of the literature. Updated constraints on the abundance of compact objects accounting for such discrepancies may be required." }, "authors": [ { "name": { - "surname": "Bosc\u00e1", - "given_name": "V\u00edctor" + "given_name": "V\u00edctor", + "surname": "Bosc\u00e1" } }, { "name": { - "surname": "Fleury", - "given_name": "Pierre" + "given_name": "Pierre", + "surname": "Fleury" } }, { "name": { - "surname": "Garc\u00eda-Bellido", - "given_name": "Juan" + "given_name": "Juan", + "surname": "Garc\u00eda-Bellido" } } ], - "title": { - "textEnglish": "Accurate modelling of extragalactic microlensing by compact objects" + "copyright": { + "statement": "\u00a9 2022 IOP Publishing Ltd and Sissa Medialab", + "status": true }, - "abstract": { - "textEnglish": "Microlensing of extragalactic sources, in particular the probability of significant amplifications, is a potentially powerful probe of the abundance of compact objects outside the halo of the Milky Way. Accurate experimental constraints require an equally accurate theoretical model for the amplification statistics produced by such a population. In this article, we argue that the simplest (strongest-lens) model does not meet this demanding requirement. We thus propose an elaborate practical modelling scheme for extragalactic microlensing. We derive from first principles an expression for the amplification probability that consistently allows for: (i) the coupling between microlenses; (ii) realistic perturbations from the cosmic large-scale structure; (iii) extended-source corrections. An important conclusion is that the external shear applied on the dominant microlens, both by the other lenses and by the large-scale structure, is practically negligible. Yet, the predictions of our approach can still differ by a factor of a few with respect to existing models of the literature. Updated constraints on the abundance of compact objects accounting for such discrepancies may be required." + "editorialHistory": { + "acceptedDate": "2022-10-16", + "receivedDates": [ + "2022-05-06" + ] + }, + "esources": [ + { + "location": "https://iopscience.iop.org/article/10.1088/1475-7516/2022/10/098", + "source": "pub_html" + } + ], + "pagination": { + "firstPage": "098" + }, + "persistentIDs": [ + { + "DOI": "10.1088/1475-7516/2022/10/098" + } + ], + "pubDate": { + "electrDate": "2022-10-31", + "printDate": "2022-10-01" + }, + "publication": { + "ISSN": [ + { + "issnString": "1475-7516", + "pubtype": "electronic" + } + ], + "issueNum": "10", + "pubName": "Journal of Cosmology and Astroparticle Physics", + "pubYear": "2022", + "volumeNum": "2022" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " Phys. Rev. Lett. Abbott 10.1103/PhysRevLett.116.241103 116 2016 GW151226: Observation of Gravitational Waves from a 22-Solar-Mass Binary Black Hole Coalescence ", @@ -157,14 +164,7 @@ "", "" ], - "esources": [ - { - "source": "pub_html", - "location": "https://iopscience.iop.org/article/10.1088/1475-7516/2022/10/098" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 2022 IOP Publishing Ltd and Sissa Medialab" + "title": { + "textEnglish": "Accurate modelling of extragalactic microlensing by compact objects" } } diff --git a/tests/stubdata/output/crossref_cn_10.1093=mnras=stac2975.json b/tests/stubdata/output/crossref_cn_10.1093=mnras=stac2975.json index 73ca4b8..7468317 100644 --- a/tests/stubdata/output/crossref_cn_10.1093=mnras=stac2975.json +++ b/tests/stubdata/output/crossref_cn_10.1093=mnras=stac2975.json @@ -1,99 +1,141 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2022-09-20", - "printDate": "2022-11-10" - }, - "publication": { - "pubName": "Monthly Notices of the Royal Astronomical Society", - "issueNum": "4", - "volumeNum": "517", - "pubYear": "2022", - "ISSN": [ - { - "pubtype": "print", - "issnString": "0035-8711" - }, - { - "pubtype": "electronic", - "issnString": "1365-2966" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1093/mnras/stac2975" - } - ], - "pagination": { - "firstPage": "5496", - "lastPage": "5523" + "abstract": { + "textEnglish": "Clustering is an effective tool for astronomical spectral analysis, to mine clustering patterns among data. With the implementation of large sky surveys, many clustering methods have been applied to tackle spectroscopic and photometric data effectively and automatically. Meanwhile, the performance of clustering methods under different data characteristics varies greatly. With the aim of summarizing astronomical spectral clustering algorithms and laying the foundation for further research, this work gives a review of clustering methods applied to astronomical spectra data in three parts. First, many clustering methods for astronomical spectra are investigated and analysed theoretically, looking at algorithmic ideas, applications, and features. Secondly, experiments are carried out on unified datasets constructed using three criteria (spectra data type, spectra quality, and data volume) to compare the performance of typical algorithms; spectra data are selected from the Large Sky Area Multi-Object Fibre Spectroscopic Telescope (LAMOST) survey and Sloan Digital Sky Survey (SDSS). Finally, source codes of the comparison clustering algorithms and manuals for usage and improvement are provided on GitHub." }, "authors": [ { "name": { - "surname": "Yang", - "given_name": "Haifeng" + "given_name": "Haifeng", + "surname": "Yang" } }, { "name": { - "surname": "Shi", - "given_name": "Chenhui" + "given_name": "Chenhui", + "surname": "Shi" } }, { - "name": { - "surname": "Cai", - "given_name": "Jianghui" - }, "attrib": { "orcid": "0000-0001-6945-8093" + }, + "name": { + "given_name": "Jianghui", + "surname": "Cai" } }, { "name": { - "surname": "Zhou", - "given_name": "Lichan" + "given_name": "Lichan", + "surname": "Zhou" } }, { "name": { - "surname": "Yang", - "given_name": "Yuqing" + "given_name": "Yuqing", + "surname": "Yang" } }, { "name": { - "surname": "Zhao", - "given_name": "Xujun" + "given_name": "Xujun", + "surname": "Zhao" } }, { "name": { - "surname": "He", - "given_name": "Yanting" + "given_name": "Yanting", + "surname": "He" } }, { "name": { - "surname": "Hao", - "given_name": "Jing" + "given_name": "Jing", + "surname": "Hao" } } ], - "title": { - "textEnglish": "Data mining techniques on astronomical spectra data \u2013 I. Clustering analysis" + "esources": [ + { + "location": "https://academic.oup.com/mnras/article/517/4/5496/6764744", + "source": "pub_html" + } + ], + "funding": [ + { + "agencyid": { + "idvalue": "http://dx.doi.org/10.13039/501100002367" + }, + "agencyname": "Chinese Academy of Sciences" + }, + { + "agencyid": { + "idvalue": "http://dx.doi.org/10.13039/501100010453" + }, + "agencyname": "National Development and Reform Commission" + }, + { + "agencyid": { + "idvalue": "http://dx.doi.org/10.13039/501100001809" + }, + "agencyname": "National Natural Science Foundation of China", + "awardnumber": "U1931209" + }, + { + "agencyid": { + "idvalue": "http://dx.doi.org/10.13039/501100013317" + }, + "agencyname": "Key Research and Development Project of Shanxi Province", + "awardnumber": "201903D121116" + }, + { + "agencyid": { + "idvalue": "http://dx.doi.org/10.13039/501100003009" + }, + "agencyname": "Science and Technology Development Fund", + "awardnumber": "20201070" + }, + { + "agencyname": "Fundamental Research Program of Shanxi Province", + "awardnumber": "20210302123223" + } + ], + "pagination": { + "firstPage": "5496", + "lastPage": "5523" }, - "abstract": { - "textEnglish": "Clustering is an effective tool for astronomical spectral analysis, to mine clustering patterns among data. With the implementation of large sky surveys, many clustering methods have been applied to tackle spectroscopic and photometric data effectively and automatically. Meanwhile, the performance of clustering methods under different data characteristics varies greatly. With the aim of summarizing astronomical spectral clustering algorithms and laying the foundation for further research, this work gives a review of clustering methods applied to astronomical spectra data in three parts. First, many clustering methods for astronomical spectra are investigated and analysed theoretically, looking at algorithmic ideas, applications, and features. Secondly, experiments are carried out on unified datasets constructed using three criteria (spectra data type, spectra quality, and data volume) to compare the performance of typical algorithms; spectra data are selected from the Large Sky Area Multi-Object Fibre Spectroscopic Telescope (LAMOST) survey and Sloan Digital Sky Survey (SDSS). Finally, source codes of the comparison clustering algorithms and manuals for usage and improvement are provided on GitHub." + "persistentIDs": [ + { + "DOI": "10.1093/mnras/stac2975" + } + ], + "pubDate": { + "electrDate": "2022-09-20", + "printDate": "2022-11-10" + }, + "publication": { + "ISSN": [ + { + "issnString": "0035-8711", + "pubtype": "print" + }, + { + "issnString": "1365-2966", + "pubtype": "electronic" + } + ], + "issueNum": "4", + "pubName": "Monthly Notices of the Royal Astronomical Society", + "pubYear": "2022", + "volumeNum": "517" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " MNRAS Acuner 475 1708 2018 10.1093/mnras/stx3106 ", @@ -209,49 +251,7 @@ " A&A Zari 628 A123 2019 10.1051/0004-6361/201935781 ", " Proc. 1996 ACM SIGMOD International Conference on Management of Data (SIGMOD\u201996 Zhang 103 1996 10.1145/233269.233324 " ], - "esources": [ - { - "source": "pub_html", - "location": "https://academic.oup.com/mnras/article/517/4/5496/6764744" - } - ], - "funding": [ - { - "agencyname": "Chinese Academy of Sciences", - "agencyid": { - "idvalue": "http://dx.doi.org/10.13039/501100002367" - } - }, - { - "agencyname": "National Development and Reform Commission", - "agencyid": { - "idvalue": "http://dx.doi.org/10.13039/501100010453" - } - }, - { - "agencyname": "National Natural Science Foundation of China", - "agencyid": { - "idvalue": "http://dx.doi.org/10.13039/501100001809" - }, - "awardnumber": "U1931209" - }, - { - "agencyname": "Key Research and Development Project of Shanxi Province", - "agencyid": { - "idvalue": "http://dx.doi.org/10.13039/501100013317" - }, - "awardnumber": "201903D121116" - }, - { - "agencyname": "Science and Technology Development Fund", - "agencyid": { - "idvalue": "http://dx.doi.org/10.13039/501100003009" - }, - "awardnumber": "20201070" - }, - { - "agencyname": "Fundamental Research Program of Shanxi Province", - "awardnumber": "20210302123223" - } - ] + "title": { + "textEnglish": "Data mining techniques on astronomical spectra data \u2013 I. Clustering analysis" + } } diff --git a/tests/stubdata/output/crossref_cn_10.1093=pasj=psac053.json b/tests/stubdata/output/crossref_cn_10.1093=pasj=psac053.json index a8399a3..a5faa64 100644 --- a/tests/stubdata/output/crossref_cn_10.1093=pasj=psac053.json +++ b/tests/stubdata/output/crossref_cn_10.1093=pasj=psac053.json @@ -1,93 +1,117 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2022-07-19", - "printDate": "2022-10-03" - }, - "publication": { - "pubName": "Publications of the Astronomical Society of Japan", - "issueNum": "5", - "volumeNum": "74", - "pubYear": "2022", - "ISSN": [ - { - "pubtype": "print", - "issnString": "0004-6264" - }, - { - "pubtype": "electronic", - "issnString": "2053-051X" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1093/pasj/psac053" - } - ], - "pagination": { - "firstPage": "1022", - "lastPage": "1040" + "abstract": { + "textEnglish": "A novel collisionless shock jump condition is suggested by modeling the entropy production at the shock transition region. We also calculate downstream developments of the atomic ionization balance and the ion temperature relaxation in supernova remnants (SNRs). The injection process and subsequent acceleration of cosmic rays (CRs) in the SNR shocks are closely related to the formation process of the collisionless shocks. The formation of the shock is caused by wave\u2013particle interactions. Since the wave\u2013particle interactions result in energy exchanges between electromagnetic fields and charged particles, the randomization of particles associated with the shock transition may occur at a rate given by the scalar product of the electric field and current. We find that order-of-magnitude estimates of the randomization with reasonable strength of the electromagnetic fields in the SNR constrain the amount of CR nuclei and the ion temperatures. The constrained amount of CR nuclei can be sufficient to explain the Galactic CRs. The ion temperature becomes significantly lower than that in the case without CRs. To distinguish the case without CRs, we perform synthetic observations of atomic line emissions from the downstream region of the SNR RCW 86. Future observations by XRISM and Athena can distinguish whether the SNR shock accelerates the CRs or not from the ion temperatures." }, "authors": [ { - "name": { - "surname": "Shimoda", - "given_name": "Jiro" - }, "attrib": { "orcid": "0000-0003-3383-2279" + }, + "name": { + "given_name": "Jiro", + "surname": "Shimoda" } }, { "name": { - "surname": "Ohira", - "given_name": "Yutaka" + "given_name": "Yutaka", + "surname": "Ohira" } }, { "name": { - "surname": "Bamba", - "given_name": "Aya" + "given_name": "Aya", + "surname": "Bamba" } }, { "name": { - "surname": "Terada", - "given_name": "Yukikatsu" + "given_name": "Yukikatsu", + "surname": "Terada" } }, { "name": { - "surname": "Yamazaki", - "given_name": "Ryo" + "given_name": "Ryo", + "surname": "Yamazaki" } }, { "name": { - "surname": "Inoue", - "given_name": "Tsuyoshi" + "given_name": "Tsuyoshi", + "surname": "Inoue" } }, { "name": { - "surname": "Tanaka", - "given_name": "Shuta J" + "given_name": "Shuta J", + "surname": "Tanaka" } } ], - "title": { - "textEnglish": "X-ray line diagnostics of ion temperature at cosmic ray accelerating collisionless shocks" + "esources": [ + { + "location": "https://academic.oup.com/pasj/article/74/5/1022/6646725", + "source": "pub_html" + } + ], + "funding": [ + { + "agencyid": { + "idvalue": "http://dx.doi.org/10.13039/501100001691" + }, + "agencyname": "JSPS", + "awardnumber": "20J01086" + }, + { + "agencyid": { + "idvalue": "http://dx.doi.org/10.13039/501100001700" + }, + "agencyname": "MEXT" + }, + { + "agencyid": { + "idvalue": "http://dx.doi.org/10.13039/501100004968" + }, + "agencyname": "Aoyama Gakuin University Research Institute" + } + ], + "pagination": { + "firstPage": "1022", + "lastPage": "1040" }, - "abstract": { - "textEnglish": "A novel collisionless shock jump condition is suggested by modeling the entropy production at the shock transition region. We also calculate downstream developments of the atomic ionization balance and the ion temperature relaxation in supernova remnants (SNRs). The injection process and subsequent acceleration of cosmic rays (CRs) in the SNR shocks are closely related to the formation process of the collisionless shocks. The formation of the shock is caused by wave\u2013particle interactions. Since the wave\u2013particle interactions result in energy exchanges between electromagnetic fields and charged particles, the randomization of particles associated with the shock transition may occur at a rate given by the scalar product of the electric field and current. We find that order-of-magnitude estimates of the randomization with reasonable strength of the electromagnetic fields in the SNR constrain the amount of CR nuclei and the ion temperatures. The constrained amount of CR nuclei can be sufficient to explain the Galactic CRs. The ion temperature becomes significantly lower than that in the case without CRs. To distinguish the case without CRs, we perform synthetic observations of atomic line emissions from the downstream region of the SNR RCW 86. Future observations by XRISM and Athena can distinguish whether the SNR shock accelerates the CRs or not from the ion temperatures." + "persistentIDs": [ + { + "DOI": "10.1093/pasj/psac053" + } + ], + "pubDate": { + "electrDate": "2022-07-19", + "printDate": "2022-10-03" + }, + "publication": { + "ISSN": [ + { + "issnString": "0004-6264", + "pubtype": "print" + }, + { + "issnString": "2053-051X", + "pubtype": "electronic" + } + ], + "issueNum": "5", + "pubName": "Publications of the Astronomical Society of Japan", + "pubYear": "2022", + "volumeNum": "74" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " ApJ Abdo 736 131 2011 10.1088/0004-637X/736/2/131 ", @@ -183,31 +207,7 @@ " A&A Zatsarinny 412 587 2003 10.1051/0004-6361:20031462 ", " A&A Zatsarinny 417 1173 2004 10.1051/0004-6361:20034174 " ], - "esources": [ - { - "source": "pub_html", - "location": "https://academic.oup.com/pasj/article/74/5/1022/6646725" - } - ], - "funding": [ - { - "agencyname": "JSPS", - "agencyid": { - "idvalue": "http://dx.doi.org/10.13039/501100001691" - }, - "awardnumber": "20J01086" - }, - { - "agencyname": "MEXT", - "agencyid": { - "idvalue": "http://dx.doi.org/10.13039/501100001700" - } - }, - { - "agencyname": "Aoyama Gakuin University Research Institute", - "agencyid": { - "idvalue": "http://dx.doi.org/10.13039/501100004968" - } - } - ] + "title": { + "textEnglish": "X-ray line diagnostics of ion temperature at cosmic ray accelerating collisionless shocks" + } } diff --git a/tests/stubdata/output/crossref_cn_10.3847=1538-4357=ac8c2f.json b/tests/stubdata/output/crossref_cn_10.3847=1538-4357=ac8c2f.json index c254832..915e1e8 100644 --- a/tests/stubdata/output/crossref_cn_10.3847=1538-4357=ac8c2f.json +++ b/tests/stubdata/output/crossref_cn_10.3847=1538-4357=ac8c2f.json @@ -1,116 +1,123 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2022-04-05" - ], - "acceptedDate": "2022-08-22" - }, - "pubDate": { - "electrDate": "2022-11-08", - "printDate": "2022-11-01" - }, - "publication": { - "pubName": "The Astrophysical Journal", - "issueNum": "2", - "volumeNum": "939", - "pubYear": "2022", - "ISSN": [ - { - "pubtype": "print", - "issnString": "0004-637X" - }, - { - "pubtype": "electronic", - "issnString": "1538-4357" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.3847/1538-4357/ac8c2f" - } - ], - "pagination": { - "firstPage": "83" + "abstract": { + "textEnglish": "Motivated by the measured velocity profile of the M87 jet using the Korean very-long-baseline interferometry (VLBI) network (KVN) and VLBI Exploration of Radio Astrometry (VERA) Array (KaVA) by Park et al. indicating that the starting position of the jet acceleration is farther from the central engine of the jet than predicted in general relativistic magnetohydrodynamic simulations, we explore how to mitigate the apparent discrepancy between the simulations and the KaVA observation. We use a semi-analytic jet model proposed by Tomimatsu & Takahashi consistently solving the transmagnetic field structure but neglecting any dissipation effects. By comparing the jet model with the observed M87 jet velocity profile, we find that the model can reproduce the logarithmic feature of the velocity profile and can fit the observed data when choosing c /(100 r g ) \u2272 \u03a9 F \u2272 c /(70 r g ), where r g is the gravitational radius. While a total specific energy ( \ue231 ) of the jet changes the terminal bulk Lorentz factor of the jet, a slower angular velocity of the black hole magnetosphere (\u03a9 F ) makes a light-cylinder radius ( r lc ) larger, and it consequently pushes out a location of a starting point of the jet acceleration. Using the estimated \u03a9 F we further estimate the magnetic field strength on the event horizon scale in M87 by assuming Blandford\u2013Znajek process is in action. The corresponding magnetic flux threading the event horizon of M87 is in good agreement with a magnetically arrested disk regime." }, "authors": [ { - "name": { - "surname": "Kino", - "given_name": "Motoki" - }, "attrib": { "orcid": "0000-0002-2709-7338" + }, + "name": { + "given_name": "Motoki", + "surname": "Kino" } }, { - "name": { - "surname": "Takahashi", - "given_name": "Masaaki" - }, "attrib": { "orcid": "0000-0001-9360-0846" + }, + "name": { + "given_name": "Masaaki", + "surname": "Takahashi" } }, { - "name": { - "surname": "Kawashima", - "given_name": "Tomohisa" - }, "attrib": { "orcid": "0000-0001-8527-0496" + }, + "name": { + "given_name": "Tomohisa", + "surname": "Kawashima" } }, { - "name": { - "surname": "Park", - "given_name": "Jongho" - }, "attrib": { "orcid": "0000-0001-6558-9053" + }, + "name": { + "given_name": "Jongho", + "surname": "Park" } }, { - "name": { - "surname": "Hada", - "given_name": "Kazuhiro" - }, "attrib": { "orcid": "0000-0001-6906-772X" + }, + "name": { + "given_name": "Kazuhiro", + "surname": "Hada" } }, { - "name": { - "surname": "Ro", - "given_name": "Hyunwook" - }, "attrib": { "orcid": "0000-0002-7322-6436" + }, + "name": { + "given_name": "Hyunwook", + "surname": "Ro" } }, { - "name": { - "surname": "Cui", - "given_name": "Yuzhu" - }, "attrib": { "orcid": "0000-0001-6311-4345" + }, + "name": { + "given_name": "Yuzhu", + "surname": "Cui" } } ], - "title": { - "textEnglish": "Implications from the Velocity Profile of the M87 Jet: A Possibility of a Slowly Rotating Black Hole Magnetosphere" + "copyright": { + "statement": "\u00a9 2022. The Author(s). Published by the American Astronomical Society.", + "status": true }, - "abstract": { - "textEnglish": "Motivated by the measured velocity profile of the M87 jet using the Korean very-long-baseline interferometry (VLBI) network (KVN) and VLBI Exploration of Radio Astrometry (VERA) Array (KaVA) by Park et al. indicating that the starting position of the jet acceleration is farther from the central engine of the jet than predicted in general relativistic magnetohydrodynamic simulations, we explore how to mitigate the apparent discrepancy between the simulations and the KaVA observation. We use a semi-analytic jet model proposed by Tomimatsu & Takahashi consistently solving the transmagnetic field structure but neglecting any dissipation effects. By comparing the jet model with the observed M87 jet velocity profile, we find that the model can reproduce the logarithmic feature of the velocity profile and can fit the observed data when choosing c /(100 r g ) \u2272 \u03a9 F \u2272 c /(70 r g ), where r g is the gravitational radius. While a total specific energy ( \ue231 ) of the jet changes the terminal bulk Lorentz factor of the jet, a slower angular velocity of the black hole magnetosphere (\u03a9 F ) makes a light-cylinder radius ( r lc ) larger, and it consequently pushes out a location of a starting point of the jet acceleration. Using the estimated \u03a9 F we further estimate the magnetic field strength on the event horizon scale in M87 by assuming Blandford\u2013Znajek process is in action. The corresponding magnetic flux threading the event horizon of M87 is in good agreement with a magnetically arrested disk regime." + "editorialHistory": { + "acceptedDate": "2022-08-22", + "receivedDates": [ + "2022-04-05" + ] + }, + "esources": [ + { + "location": "https://iopscience.iop.org/article/10.3847/1538-4357/ac8c2f", + "source": "pub_html" + } + ], + "pagination": { + "firstPage": "83" + }, + "persistentIDs": [ + { + "DOI": "10.3847/1538-4357/ac8c2f" + } + ], + "pubDate": { + "electrDate": "2022-11-08", + "printDate": "2022-11-01" + }, + "publication": { + "ISSN": [ + { + "issnString": "0004-637X", + "pubtype": "print" + }, + { + "issnString": "1538-4357", + "pubtype": "electronic" + } + ], + "issueNum": "2", + "pubName": "The Astrophysical Journal", + "pubYear": "2022", + "volumeNum": "939" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " ApJ Abramowski 10.1088/0004-637X/746/2/151 746 151 2012 ", @@ -227,14 +234,7 @@ " Natur Zamaninasab 10.1038/nature13399 510 126 2014 ", " MNRAS Znajek 10.1093/mnras/179.3.457 179 457 1977 " ], - "esources": [ - { - "source": "pub_html", - "location": "https://iopscience.iop.org/article/10.3847/1538-4357/ac8c2f" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 2022. The Author(s). Published by the American Astronomical Society." + "title": { + "textEnglish": "Implications from the Velocity Profile of the M87 Jet: A Possibility of a Slowly Rotating Black Hole Magnetosphere" } } diff --git a/tests/stubdata/output/crossref_conf_10.1049-cp.2010.1342.json b/tests/stubdata/output/crossref_conf_10.1049-cp.2010.1342.json index eca0964..53d2c1f 100644 --- a/tests/stubdata/output/crossref_conf_10.1049-cp.2010.1342.json +++ b/tests/stubdata/output/crossref_conf_10.1049-cp.2010.1342.json @@ -1,38 +1,4 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "printDate": "2010-00-00" - }, - "publication": { - "pubName": "International Conference on Advanced Technology of Design and Manufacture (ATDM 2010)", - "confName": "International Conference on Advanced Technology of Design and Manufacture (ATDM 2010)", - "confLocation": "Beijing, China", - "confDates": "23-25 Nov. 2010", - "publisher": "IET", - "pubYear": "2010" - }, - "persistentIDs": [ - { - "ISBN": [ - { - "pubtype": "print", - "isbnString": "978 1 84919 238 5" - } - ], - "DOI": "10.1049/cp.2010.1342" - } - ], - "pagination": { - "firstPage": "447", - "lastPage": "449" - }, "authors": [ { "name": { @@ -55,13 +21,47 @@ } } ], - "title": { - "textEnglish": "Analysis of electrochemical degradation of coking wastewater using multiwall carbon nanotubes modified electrode" - }, "esources": [ { - "source": "pub_html", - "location": "https://digital-library.theiet.org/content/conferences/10.1049/cp.2010.1342" + "location": "https://digital-library.theiet.org/content/conferences/10.1049/cp.2010.1342", + "source": "pub_html" } - ] + ], + "pagination": { + "firstPage": "447", + "lastPage": "449" + }, + "persistentIDs": [ + { + "DOI": "10.1049/cp.2010.1342", + "ISBN": [ + { + "isbnString": "978 1 84919 238 5", + "pubtype": "print" + } + ] + } + ], + "pubDate": { + "printDate": "2010-00-00" + }, + "publication": { + "confDates": "23-25 Nov. 2010", + "confLocation": "Beijing, China", + "confName": "International Conference on Advanced Technology of Design and Manufacture (ATDM 2010)", + "pubName": "International Conference on Advanced Technology of Design and Manufacture (ATDM 2010)", + "pubYear": "2010", + "publisher": "IET" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "title": { + "textEnglish": "Analysis of electrochemical degradation of coking wastewater using multiwall carbon nanotubes modified electrode" + } } diff --git a/tests/stubdata/output/crossref_conf_10.1109-MWSYM.2013.6697399.json b/tests/stubdata/output/crossref_conf_10.1109-MWSYM.2013.6697399.json index 8d76ef4..111b2d7 100644 --- a/tests/stubdata/output/crossref_conf_10.1109-MWSYM.2013.6697399.json +++ b/tests/stubdata/output/crossref_conf_10.1109-MWSYM.2013.6697399.json @@ -1,112 +1,112 @@ { - 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"name": { - "surname": "Tessmann", - "given_name": "Axel" - }, "affiliation": [ { "affPubRaw": "Fraunhofer IAF, Freiburg, Germany Universita\u00a8t Stuttgart, Institute of Robust Power Semiconductor Systems, Stuttgart, Germany" } - ] + ], + "name": { + "given_name": "Axel", + "surname": "Tessmann" + } }, { - "name": { - "surname": "Massler", - "given_name": "Hermann" - }, "affiliation": [ { "affPubRaw": "Fraunhofer IAF, Freiburg, Germany Universita\u00a8t Stuttgart, Institute of Robust Power Semiconductor Systems, Stuttgart, Germany" } - ] + ], + "name": { + "given_name": "Hermann", + "surname": "Massler" + } }, { - "name": { - "surname": "Leuther", - "given_name": "Arnulf" - }, "affiliation": [ { "affPubRaw": "Fraunhofer IAF, Freiburg, Germany Universita\u00a8t Stuttgart, Institute of Robust Power Semiconductor Systems, Stuttgart, Germany" } - ] + ], + "name": { + "given_name": "Arnulf", + "surname": "Leuther" + } }, { - "name": { - "surname": "Zwick", - "given_name": "Thomas" - }, "affiliation": [ { "affPubRaw": "Karlsruhe Institute of Technology (KIT), Institut fu\u00a8r Hochfrequenztechnik und Elektronik, Karlsruhe, Germany" } - ] + ], + "name": { + "given_name": "Thomas", + "surname": "Zwick" + } }, { - "name": { - "surname": "Kallfass", - "given_name": "Ingmar" - }, "affiliation": [ { "affPubRaw": "Fraunhofer IAF, Freiburg, Germany Universita\u00a8t Stuttgart, Institute of Robust Power Semiconductor Systems, Stuttgart, Germany" } - ] + ], + "name": { + "given_name": "Ingmar", + "surname": "Kallfass" + } } ], - "title": { - "textEnglish": "An active 600 GHz frequency multiplier-by-six S-MMIC" - }, "esources": [ { - "source": "pub_html", - "location": "https://ieeexplore.ieee.org/document/6697399/" + "location": "https://ieeexplore.ieee.org/document/6697399/", + "source": "pub_html" } - ] + ], + "pagination": { + "firstPage": "1", + "lastPage": "3" + }, + "persistentIDs": [ + { + "DOI": "10.1109/MWSYM.2013.6697399", + "ISBN": [ + { + "isbnString": "978-1-4673-6176-7", + "pubtype": "electronic" + } + ] + } + ], + "pubDate": { + "printDate": "2013-06-00" + }, + "publication": { + "confLocation": "Seattle, WA, USA", + "confName": "2013 IEEE/MTT-S International Microwave Symposium - MTT 2013", + "pubName": "2013 IEEE MTT-S International Microwave Symposium Digest (MTT)", + "pubYear": "2013", + "publisher": "IEEE" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "title": { + "textEnglish": "An active 600 GHz frequency multiplier-by-six S-MMIC" + } } diff --git a/tests/stubdata/output/crossref_preprint_10.1002-essoar.10508651.1.json b/tests/stubdata/output/crossref_preprint_10.1002-essoar.10508651.1.json index 72853fc..42a2306 100644 --- a/tests/stubdata/output/crossref_preprint_10.1002-essoar.10508651.1.json +++ b/tests/stubdata/output/crossref_preprint_10.1002-essoar.10508651.1.json @@ -1,30 +1,6 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2021-11-08" - }, - "publication": { - "publisher": "Earth and Space Science Open Archive (ESSOAr)", - "pubYear": "2021" - }, - "persistentIDs": [ - { - "DOI": "10.1002/essoar.10508651.1" - } - ], "authors": [ { - "name": { - "surname": "Livi", - "given_name": "Roberto" - }, "affiliation": [ { "affPubRaw": "University of California" @@ -32,24 +8,24 @@ ], "attrib": { "orcid": "0000-0002-0396-0547" + }, + "name": { + "given_name": "Roberto", + "surname": "Livi" } }, { - "name": { - "surname": "Larson", - "given_name": "Davin E" - }, "affiliation": [ { "affPubRaw": "University of California" } - ] + ], + "name": { + "given_name": "Davin E", + "surname": "Larson" + } }, { - "name": { - "surname": "Kasper", - "given_name": "Justin C" - }, "affiliation": [ { "affPubRaw": "University of Michigan" @@ -57,35 +33,35 @@ { "affPubRaw": "Smithsonian Astrophysical Observatory" } - ] + ], + "name": { + "given_name": "Justin C", + "surname": "Kasper" + } }, { - "name": { - "surname": "Abiad", - "given_name": "Robert" - }, "affiliation": [ { "affPubRaw": "University of California" } - ] + ], + "name": { + "given_name": "Robert", + "surname": "Abiad" + } }, { - "name": { - "surname": "Case", - "given_name": "Anthony W" - }, "affiliation": [ { "affPubRaw": "Smithsonian Astrophysical Observatory" } - ] + ], + "name": { + "given_name": "Anthony W", + "surname": "Case" + } }, { - "name": { - "surname": "Klein", - "given_name": "Kristopher G" - }, "affiliation": [ { "affPubRaw": "University of Michigan" @@ -93,190 +69,214 @@ { "affPubRaw": "University of Arizona" } - ] + ], + "name": { + "given_name": "Kristopher G", + "surname": "Klein" + } }, { - "name": { - "surname": "Curtis", - "given_name": "David W" - }, "affiliation": [ { "affPubRaw": "University of California" } - ] + ], + "name": { + "given_name": "David W", + "surname": "Curtis" + } }, { - "name": { - "surname": "Dalton", - "given_name": "Gregory" - }, "affiliation": [ { "affPubRaw": "University of California" } - ] + ], + "name": { + "given_name": "Gregory", + "surname": "Dalton" + } }, { - "name": { - "surname": "Stevens", - "given_name": "Michael" - }, "affiliation": [ { "affPubRaw": "Smithsonian Astrophysical Observatory" } - ] + ], + "name": { + "given_name": "Michael", + "surname": "Stevens" + } }, { - "name": { - "surname": "Korreck", - "given_name": "Kelly E" - }, "affiliation": [ { "affPubRaw": "Smithsonian Astrophysical Observatory" } - ] + ], + "name": { + "given_name": "Kelly E", + "surname": "Korreck" + } }, { - "name": { - "surname": "Ho", - "given_name": "George" - }, "affiliation": [ { "affPubRaw": "Applied Physics Laboratory, Johns Hopkins University" } - ] + ], + "name": { + "given_name": "George", + "surname": "Ho" + } }, { - "name": { - "surname": "Robinson", - "given_name": "Miles" - }, "affiliation": [ { "affPubRaw": "University of California" } - ] + ], + "name": { + "given_name": "Miles", + "surname": "Robinson" + } }, { - "name": { - "surname": "Tiu", - "given_name": "Chris" - }, "affiliation": [ { "affPubRaw": "NASA" } - ] + ], + "name": { + "given_name": "Chris", + "surname": "Tiu" + } }, { - "name": { - "surname": "Whittlesey", - "given_name": "Phyllis L" - }, "affiliation": [ { "affPubRaw": "University of California" } - ] + ], + "name": { + "given_name": "Phyllis L", + "surname": "Whittlesey" + } }, { - "name": { - "surname": "Verniero", - "given_name": "J L" - }, "affiliation": [ { "affPubRaw": "University of California" } - ] + ], + "name": { + "given_name": "J L", + "surname": "Verniero" + } }, { - "name": { - "surname": "Halekas", - "given_name": "Jasper" - }, "affiliation": [ { "affPubRaw": "University of Iowa" } - ] + ], + "name": { + "given_name": "Jasper", + "surname": "Halekas" + } }, { - "name": { - "surname": "Mcfadden", - "given_name": "James" - }, "affiliation": [ { "affPubRaw": "University of California" } - ] + ], + "name": { + "given_name": "James", + "surname": "Mcfadden" + } }, { - "name": { - "surname": "Marckwordt", - "given_name": "Mario" - }, "affiliation": [ { "affPubRaw": "University of California" } - ] + ], + "name": { + "given_name": "Mario", + "surname": "Marckwordt" + } }, { - "name": { - "surname": "Slagle", - "given_name": "Amanda" - }, "affiliation": [ { "affPubRaw": "University of California" } - ] + ], + "name": { + "given_name": "Amanda", + "surname": "Slagle" + } }, { - "name": { - "surname": "Abatcha", - "given_name": "Mamuda" - }, "affiliation": [ { "affPubRaw": "University of California" } - ] + ], + "name": { + "given_name": "Mamuda", + "surname": "Abatcha" + } }, { - "name": { - "surname": "Rahmati", - "given_name": "Ali" - }, "affiliation": [ { "affPubRaw": "University of California" } - ] + ], + "name": { + "given_name": "Ali", + "surname": "Rahmati" + } } ], - "title": { - "textEnglish": "The Solar Probe ANalyzer -Ions on Parker Solar Probe" - }, "esources": [ { - "source": "pub_html", - "location": "https://essopenarchive.org/doi/full/10.1002/essoar.10508651.1" + "location": "https://essopenarchive.org/doi/full/10.1002/essoar.10508651.1", + "source": "pub_html" } ], "funding": [ { - "agencyname": "National Aeronautics and Space Administration", "agencyid": { "idvalue": "100000104" }, + "agencyname": "National Aeronautics and Space Administration", "awardnumber": "NNN06AA01C" } - ] + ], + "persistentIDs": [ + { + "DOI": "10.1002/essoar.10508651.1" + } + ], + "pubDate": { + "electrDate": "2021-11-08" + }, + "publication": { + "pubYear": "2021", + "publisher": "Earth and Space Science Open Archive (ESSOAr)" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "title": { + "textEnglish": "The Solar Probe ANalyzer -Ions on Parker Solar Probe" + } } diff --git a/tests/stubdata/output/crossref_preprint_10.1002-essoar.10511074.2.json b/tests/stubdata/output/crossref_preprint_10.1002-essoar.10511074.2.json index 49ec262..9445f76 100644 --- a/tests/stubdata/output/crossref_preprint_10.1002-essoar.10511074.2.json +++ b/tests/stubdata/output/crossref_preprint_10.1002-essoar.10511074.2.json @@ -1,30 +1,6 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2022-04-11" - }, - "publication": { - "publisher": "Earth and Space Science Open Archive (ESSOAr)", - "pubYear": "2022" - }, - "persistentIDs": [ - { - "DOI": "10.1002/essoar.10511074.2" - } - ], "authors": [ { - "name": { - "surname": "Drilleau", - "given_name": "M\u00e9lanie" - }, "affiliation": [ { "affPubRaw": "31400 Toulouse" @@ -41,137 +17,161 @@ ], "attrib": { "orcid": "0000-0001-5625-9706" + }, + "name": { + "given_name": "M\u00e9lanie", + "surname": "Drilleau" } }, { - "name": { - "surname": "Samuel", - "given_name": "Henri" - }, "affiliation": [ { "affPubRaw": "Institut de Physique du Globe de Paris, CNRS, Universit\u00e9 de Paris, 1 rue Jussieu, 75005 Paris - France" } - ] + ], + "name": { + "given_name": "Henri", + "surname": "Samuel" + } }, { - "name": { - "surname": "Garcia", - "given_name": "Rapha\u00ebl F." - }, "affiliation": [ { "affPubRaw": "Institut Sup\u00e9rieur de l\u2019A\u00e9ronautique et de l\u2019Espace ISAE-SUPAERO, 10 Avenue Edouard Belin, 31400 Toulouse, France" } - ] + ], + "name": { + "given_name": "Rapha\u00ebl F.", + "surname": "Garcia" + } }, { - "name": { - "surname": "Rivoldini", - "given_name": "Attilio" - }, "affiliation": [ { "affPubRaw": "Royal Observatory of Belgium, Brussels, Belgium" } - ] + ], + "name": { + "given_name": "Attilio", + "surname": "Rivoldini" + } }, { - "name": { - "surname": "Perrin", - "given_name": "Cl\u00e9ment" - }, "affiliation": [ { "affPubRaw": "Nantes Universit\u00e9, Universit\u00e9 d\u2019Angers, Le Mans Universit\u00e9, CNRS UMR 6112, Laboratoire de Plan\u00e9tologie et G\u00e9osciences, UAR 3281, Observatoire des Sciences de l\u2019Univers de Nantes Atlantique, F-44000 Nantes, France" } - ] + ], + "name": { + "given_name": "Cl\u00e9ment", + "surname": "Perrin" + } }, { - "name": { - "surname": "Michaut", - "given_name": "Chlo\u00e9" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 de Lyon, Ecole Normale Sup\u00e9rieure de Lyon, Universit\u00e9 Claude Bernard Lyon 1, CNRS, Laboratoire de G\u00e9ologie de Lyon : Terre, Plan\u00e8tes, Environnement, 69622 Villeurbanne, France" } - ] + ], + "name": { + "given_name": "Chlo\u00e9", + "surname": "Michaut" + } }, { - "name": { - "surname": "Wieczorek", - "given_name": "Mark" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 C\u00f4te d\u2019Azur, Observatoire de la C\u00f4te d\u2019Azur, CNRS, Laboratoire Lagrange, France." } - ] + ], + "name": { + "given_name": "Mark", + "surname": "Wieczorek" + } }, { - "name": { - "surname": "Tauzin", - "given_name": "Beno\u00eet" - }, "affiliation": [ { "affPubRaw": "Universit\u00e9 de Lyon, Ecole Normale Sup\u00e9rieure de Lyon, Universit\u00e9 Claude Bernard Lyon 1, CNRS, Laboratoire de G\u00e9ologie de Lyon : Terre, Plan\u00e8tes, Environnement, 69622 Villeurbanne, France" } - ] + ], + "name": { + "given_name": "Beno\u00eet", + "surname": "Tauzin" + } }, { - "name": { - "surname": "Connolly", - "given_name": "James A. D." - }, "affiliation": [ { "affPubRaw": "Institute of Geophysics, ETH Zurich, Sonneggstrasse 5, Zurich, Switzerland" } - ] + ], + "name": { + "given_name": "James A. D.", + "surname": "Connolly" + } }, { - "name": { - "surname": "Meyer", - "given_name": "Pauline" - }, "affiliation": [ { "affPubRaw": "Ecole et Observatoire des Sciences de la Terre, Universit\u00e9 de Strasbourg, 5 rue Ren\u00e9 Descartes, 67084 Strasbourg, France" } - ] + ], + "name": { + "given_name": "Pauline", + "surname": "Meyer" + } }, { - "name": { - "surname": "Lognonn\u00e9", - "given_name": "Philippe" - }, "affiliation": [ { "affPubRaw": "Institut de Physique du Globe de Paris, CNRS, Universit\u00e9 de Paris, 1 rue Jussieu, 75005 Paris - France" } - ] + ], + "name": { + "given_name": "Philippe", + "surname": "Lognonn\u00e9" + } }, { - "name": { - "surname": "Banerdt", - "given_name": "William B." - }, "affiliation": [ { "affPubRaw": "Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena, CA 91109, USA" } - ] + ], + "name": { + "given_name": "William B.", + "surname": "Banerdt" + } } ], - "title": { - "textEnglish": "Marsquake locations and 1-D seismic models for Mars from InSight data" - }, "esources": [ { - "source": "pub_html", - "location": "https://essopenarchive.org/doi/full/10.1002/essoar.10511074.2" + "location": "https://essopenarchive.org/doi/full/10.1002/essoar.10511074.2", + "source": "pub_html" } - ] + ], + "persistentIDs": [ + { + "DOI": "10.1002/essoar.10511074.2" + } + ], + "pubDate": { + "electrDate": "2022-04-11" + }, + "publication": { + "pubYear": "2022", + "publisher": "Earth and Space Science Open Archive (ESSOAr)" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "title": { + "textEnglish": "Marsquake locations and 1-D seismic models for Mars from InSight data" + } } diff --git a/tests/stubdata/output/crossref_preprint_10.31223-X55K7G.json b/tests/stubdata/output/crossref_preprint_10.31223-X55K7G.json index ab36024..300c5d8 100644 --- a/tests/stubdata/output/crossref_preprint_10.31223-X55K7G.json +++ b/tests/stubdata/output/crossref_preprint_10.31223-X55K7G.json @@ -1,110 +1,110 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2021-08-06" - }, - "publication": { - "pubYear": "2021" + "abstract": { + "textEnglish": "Near-term forecasts of environmental outcomes can inform real-time decision making. Data assimilation modeling techniques can be used for forecasts to leverage real-time data streams, where the difference between model predictions and observations can be used to adjust the model to make better predictions tomorrow. In this use case, we developed a process-guided deep learning and data assimilation approach to make 7-day forecasts of daily maximum water temperature in the Delaware River Basin. Our modeling system produced forecasts of daily maximum stream temperature with an average root mean squared error (RMSE) from 1.2 to 1.6\u00b0C for 1-day lead time across all sites. The data assimilation algorithm successfully adjusted the process-guided deep learning model states and marginally improved forecast performance when compared to forecasts produced using the process-guided deep learning model alone (7-13% lower RMSE with the data assimilation algorithm). Our model characterized forecast uncertainty relatively well as 57-80% of observations were within 90% forecast confidence intervals across all sites and lead times, and the uncertainty associated with our forecasts allow managers to anticipate probability of exceedances of ecologically relevant thresholds and aid in decisions about releasing reservoir water downstream. The flexibility of deep learning models to be applied to various prediction problems shows promise for using these types of models to forecast many other important environmental variables and aid in decision making." }, - "persistentIDs": [ - { - "DOI": "10.31223/X55K7G" - } - ], "authors": [ { - "name": { - "surname": "Zwart", - "given_name": "Jacob" - }, "attrib": { "orcid": "0000-0002-3870-405X" + }, + "name": { + "given_name": "Jacob", + "surname": "Zwart" } }, { - "name": { - "surname": "Oliver", - "given_name": "Samantha" - }, "attrib": { "orcid": "0000-0001-5668-1165" + }, + "name": { + "given_name": "Samantha", + "surname": "Oliver" } }, { - "name": { - "surname": "Watkins", - "given_name": "William" - }, "attrib": { "orcid": "0000-0002-7544-0700" + }, + "name": { + "given_name": "William", + "surname": "Watkins" } }, { - "name": { - "surname": "Sadler", - "given_name": "Jeffrey" - }, "attrib": { "orcid": "0000-0001-8776-4844" + }, + "name": { + "given_name": "Jeffrey", + "surname": "Sadler" } }, { - "name": { - "surname": "Appling", - "given_name": "Alison" - }, "attrib": { "orcid": "0000-0003-3638-8572" + }, + "name": { + "given_name": "Alison", + "surname": "Appling" } }, { - "name": { - "surname": "Corson-Dosch", - "given_name": "Hayley" - }, "attrib": { "orcid": "0000-0001-8695-1584" + }, + "name": { + "given_name": "Hayley", + "surname": "Corson-Dosch" } }, { - "name": { - "surname": "Jia", - "given_name": "Xiaowei" - }, "attrib": { "orcid": "0000-0001-8544-5233" + }, + "name": { + "given_name": "Xiaowei", + "surname": "Jia" } }, { "name": { - "surname": "Kumar", - "given_name": "Vipin" + "given_name": "Vipin", + "surname": "Kumar" } }, { "name": { - "surname": "Read", - "given_name": "Jordan" + "given_name": "Jordan", + "surname": "Read" } } ], - "title": { - "textEnglish": "Near-term forecasts of stream temperature using process-guided deep learning and data assimilation" - }, - "abstract": { - "textEnglish": "Near-term forecasts of environmental outcomes can inform real-time decision making. Data assimilation modeling techniques can be used for forecasts to leverage real-time data streams, where the difference between model predictions and observations can be used to adjust the model to make better predictions tomorrow. In this use case, we developed a process-guided deep learning and data assimilation approach to make 7-day forecasts of daily maximum water temperature in the Delaware River Basin. Our modeling system produced forecasts of daily maximum stream temperature with an average root mean squared error (RMSE) from 1.2 to 1.6\u00b0C for 1-day lead time across all sites. The data assimilation algorithm successfully adjusted the process-guided deep learning model states and marginally improved forecast performance when compared to forecasts produced using the process-guided deep learning model alone (7-13% lower RMSE with the data assimilation algorithm). Our model characterized forecast uncertainty relatively well as 57-80% of observations were within 90% forecast confidence intervals across all sites and lead times, and the uncertainty associated with our forecasts allow managers to anticipate probability of exceedances of ecologically relevant thresholds and aid in decisions about releasing reservoir water downstream. The flexibility of deep learning models to be applied to various prediction problems shows promise for using these types of models to forecast many other important environmental variables and aid in decision making." - }, "esources": [ { - "source": "pub_html", - "location": "http://eartharxiv.org/repository/view/2590/" + "location": "http://eartharxiv.org/repository/view/2590/", + "source": "pub_html" + } + ], + "persistentIDs": [ + { + "DOI": "10.31223/X55K7G" } - ] + ], + "pubDate": { + "electrDate": "2021-08-06" + }, + "publication": { + "pubYear": "2021" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "title": { + "textEnglish": "Near-term forecasts of stream temperature using process-guided deep learning and data assimilation" + } } diff --git a/tests/stubdata/output/crossref_preprint_10.31223-X5FW25.json b/tests/stubdata/output/crossref_preprint_10.31223-X5FW25.json index 3f4e054..cd18072 100644 --- a/tests/stubdata/output/crossref_preprint_10.31223-X5FW25.json +++ b/tests/stubdata/output/crossref_preprint_10.31223-X5FW25.json @@ -1,236 +1,236 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2022-01-31" - }, - "publication": { - "pubYear": "2022" + "abstract": { + "textEnglish": "Four first-order (Hadean, Archean, Proterozoic and Phanerozoic eon) and nine second-order (Paleoarchean, Mesoarchean, Neoarchean, Paleoproterozoic, Mesoproterozoic, Neoproterozoic, Paleozoic, Mesozoic and Cenozoic era) units continue to provide intuitive subdivision of geological time. Major transitions in Earth\u2019s tectonic, biological and environmental history occurred at approximately 2.5-2.3, 1.8-1.6, 1.0-0.8 and 0.7-0.5 Ga, and so future rock-based subdivision of pre-Cryogenian time, eventually by use of global stratotypes (GSSPs), will likely require only modest deviation from current chronometric boundaries (GSSAs) at 2.5, 1.6 and 1.0 Ga, respectively. Here we argue that removal of GSSAs could be expedited by establishing event-based concepts and provisional, approximate ages for eon-, era- and period-level subdivisions as soon as practicable, in line with ratification of an Ediacaran GSSP in 2004 and chronostratigraphic definition of the Cryogenian Period at c. 720 Ma in 2012. We also outline the geological basis behind current chronometric divisions, explore how they might differ in any future rock-based scheme, identify where major issues might arise during the transition, and outline where some immediate changes to the present scheme could be easily updated/formalised, as a framework for future GSSP development. In line with these aims, we note that the currently recommended four-fold Archean subdivision has not been formally ratified and agree with previous workers that it could be simplified to an informal three-fold subdivision, pending more detailed analysis. Although the ages of period boundaries would inevitably change in a more closely rock-based or chronostratigraphic scheme, we support retention of all currently ratified period names. Existing period names, borrowed from the Greek, were chosen to delimit natural phenomena of global reach. Any new global nomenclature ought to follow this lead for consistency, and so we discourage the use of supercontinent names (e.g. Rodinian, Columbian) and regional phenomena, however exceptional. In this regard, we tentatively suggest that a new period (e.g. the \u2018Kratian\u2019), could precede the Tonian as the first period of the Neoproterozoic Era and we concur with previous authors that the existing Siderian Period (named for banded iron formations) would fit better as a chronostratigraphically defined period of the terminal Archean. Indeed, all pre-Cryogenian subdivisions will need more conceptual grounding in any future chronostratigraphic scheme. We conclude that improved rock-based division of the Proterozoic Eon would likely comprise a three-fold, period-level subdivision of the Paleoproterozoic Era (Oxygenian Rhyacian, Orosirian), a four-fold subdivision of the Mesoproterozoic Era (Statherian, Calymmian, Ectasian, Stenian) and potentially four-fold subdivision of the Neoproterozoic Era (pre-Tonian \u2018Kratian\u2019, Tonian, Cryogenian and Ediacaran). Future refinements towards an improved rock-based pre-Cryogenian geological time scale could be propoosed by new international bodies to cover the 1) pre-Ediacaran Neoproterozoic, 2) Mesoproterozoic, 3) Paleoproterozoic and 4) Archean (and Hadean) as few experts and disciplines can speak to the entire pre-Cryogenian rock record." }, - "persistentIDs": [ - { - "DOI": "10.31223/X5FW25" - } - ], "authors": [ { - "name": { - "surname": "Shields", - "given_name": "Graham" - }, "attrib": { "orcid": "0000-0002-7828-3966" + }, + "name": { + "given_name": "Graham", + "surname": "Shields" } }, { "name": { - "surname": "Strachan", - "given_name": "Robin" + "given_name": "Robin", + "surname": "Strachan" } }, { "name": { - "surname": "Porter", - "given_name": "Susannah" + "given_name": "Susannah", + "surname": "Porter" } }, { "name": { - "surname": "Halverson", - "given_name": "Galen" + "given_name": "Galen", + "surname": "Halverson" } }, { "name": { - "surname": "Macdonald", - "given_name": "Francis" + "given_name": "Francis", + "surname": "Macdonald" } }, { "name": { - "surname": "Plumb", - "given_name": "Kenneth" + "given_name": "Kenneth", + "surname": "Plumb" } }, { "name": { - "surname": "de Alvarenga", - "given_name": "Carlos" + "given_name": "Carlos", + "surname": "de Alvarenga" } }, { "name": { - "surname": "Banerjee", - "given_name": "Dhiraj" + "given_name": "Dhiraj", + "surname": "Banerjee" } }, { "name": { - "surname": "Bekker", - "given_name": "Andrey" + "given_name": "Andrey", + "surname": "Bekker" } }, { "name": { - "surname": "Brasier", - "given_name": "Alexander" + "given_name": "Alexander", + "surname": "Brasier" } }, { "name": { - "surname": "Chakraborty", - "given_name": "Partha" + "given_name": "Partha", + "surname": "Chakraborty" } }, { "name": { - "surname": "Condie", - "given_name": "Kent" + "given_name": "Kent", + "surname": "Condie" } }, { "name": { - "surname": "Das", - "given_name": "Kaushik" + "given_name": "Kaushik", + "surname": "Das" } }, { "name": { - "surname": "Ernst", - "given_name": "Richard" + "given_name": "Richard", + "surname": "Ernst" } }, { "name": { - "surname": "Fallick", - "given_name": "Anthony" + "given_name": "Anthony", + "surname": "Fallick" } }, { "name": { - "surname": "Frimmel", - "given_name": "Hartwig" + "given_name": "Hartwig", + "surname": "Frimmel" } }, { "name": { - "surname": "Fuck", - "given_name": "Reinhardt" + "given_name": "Reinhardt", + "surname": "Fuck" } }, { "name": { - "surname": "Hoffman", - "given_name": "Paul" + "given_name": "Paul", + "surname": "Hoffman" } }, { "name": { - "surname": "Kamber", - "given_name": "Balz" + "given_name": "Balz", + "surname": "Kamber" } }, { "name": { - "surname": "Kuznetsov", - "given_name": "Anton" + "given_name": "Anton", + "surname": "Kuznetsov" } }, { "name": { - "surname": "Mitchell", - "given_name": "Ross" + "given_name": "Ross", + "surname": "Mitchell" } }, { "name": { - "surname": "Poire", - "given_name": "Daniel" + "given_name": "Daniel", + "surname": "Poire" } }, { "name": { - "surname": "Poulton", - "given_name": "Simon" + "given_name": "Simon", + "surname": "Poulton" } }, { "name": { - "surname": "Riding", - "given_name": "Robert" + "given_name": "Robert", + "surname": "Riding" } }, { "name": { - "surname": "Sharma", - "given_name": "Mukund" + "given_name": "Mukund", + "surname": "Sharma" } }, { "name": { - "surname": "Storey", - "given_name": "Craig" + "given_name": "Craig", + "surname": "Storey" } }, { "name": { - "surname": "Stueeken", - "given_name": "Eva" + "given_name": "Eva", + "surname": "Stueeken" } }, { "name": { - "surname": "Tostevin", - "given_name": "Rosalie" + "given_name": "Rosalie", + "surname": "Tostevin" } }, { "name": { - "surname": "Turner", - "given_name": "Elizabeth" + "given_name": "Elizabeth", + "surname": "Turner" } }, { "name": { - "surname": "Xiao", - "given_name": "Shuhai" + "given_name": "Shuhai", + "surname": "Xiao" } }, { "name": { - "surname": "Zhang", - "given_name": "Shuanhong" + "given_name": "Shuanhong", + "surname": "Zhang" } }, { "name": { - "surname": "Zhou", - "given_name": "Ying" + "given_name": "Ying", + "surname": "Zhou" } }, { "name": { - "surname": "Zhu", - "given_name": "Maoyan" + "given_name": "Maoyan", + "surname": "Zhu" } } ], - "title": { - "textEnglish": "Towards a new geological time scale: A template for improved rock-based subdivision of pre-Cryogenian time" - }, - "abstract": { - "textEnglish": "Four first-order (Hadean, Archean, Proterozoic and Phanerozoic eon) and nine second-order (Paleoarchean, Mesoarchean, Neoarchean, Paleoproterozoic, Mesoproterozoic, Neoproterozoic, Paleozoic, Mesozoic and Cenozoic era) units continue to provide intuitive subdivision of geological time. Major transitions in Earth\u2019s tectonic, biological and environmental history occurred at approximately 2.5-2.3, 1.8-1.6, 1.0-0.8 and 0.7-0.5 Ga, and so future rock-based subdivision of pre-Cryogenian time, eventually by use of global stratotypes (GSSPs), will likely require only modest deviation from current chronometric boundaries (GSSAs) at 2.5, 1.6 and 1.0 Ga, respectively. Here we argue that removal of GSSAs could be expedited by establishing event-based concepts and provisional, approximate ages for eon-, era- and period-level subdivisions as soon as practicable, in line with ratification of an Ediacaran GSSP in 2004 and chronostratigraphic definition of the Cryogenian Period at c. 720 Ma in 2012. We also outline the geological basis behind current chronometric divisions, explore how they might differ in any future rock-based scheme, identify where major issues might arise during the transition, and outline where some immediate changes to the present scheme could be easily updated/formalised, as a framework for future GSSP development. In line with these aims, we note that the currently recommended four-fold Archean subdivision has not been formally ratified and agree with previous workers that it could be simplified to an informal three-fold subdivision, pending more detailed analysis. Although the ages of period boundaries would inevitably change in a more closely rock-based or chronostratigraphic scheme, we support retention of all currently ratified period names. Existing period names, borrowed from the Greek, were chosen to delimit natural phenomena of global reach. Any new global nomenclature ought to follow this lead for consistency, and so we discourage the use of supercontinent names (e.g. Rodinian, Columbian) and regional phenomena, however exceptional. In this regard, we tentatively suggest that a new period (e.g. the \u2018Kratian\u2019), could precede the Tonian as the first period of the Neoproterozoic Era and we concur with previous authors that the existing Siderian Period (named for banded iron formations) would fit better as a chronostratigraphically defined period of the terminal Archean. Indeed, all pre-Cryogenian subdivisions will need more conceptual grounding in any future chronostratigraphic scheme. We conclude that improved rock-based division of the Proterozoic Eon would likely comprise a three-fold, period-level subdivision of the Paleoproterozoic Era (Oxygenian Rhyacian, Orosirian), a four-fold subdivision of the Mesoproterozoic Era (Statherian, Calymmian, Ectasian, Stenian) and potentially four-fold subdivision of the Neoproterozoic Era (pre-Tonian \u2018Kratian\u2019, Tonian, Cryogenian and Ediacaran). Future refinements towards an improved rock-based pre-Cryogenian geological time scale could be propoosed by new international bodies to cover the 1) pre-Ediacaran Neoproterozoic, 2) Mesoproterozoic, 3) Paleoproterozoic and 4) Archean (and Hadean) as few experts and disciplines can speak to the entire pre-Cryogenian rock record." - }, "esources": [ { - "source": "pub_html", - "location": "http://eartharxiv.org/repository/view/1712/" + "location": "http://eartharxiv.org/repository/view/1712/", + "source": "pub_html" } - ] + ], + "persistentIDs": [ + { + "DOI": "10.31223/X5FW25" + } + ], + "pubDate": { + "electrDate": "2022-01-31" + }, + "publication": { + "pubYear": "2022" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "title": { + "textEnglish": "Towards a new geological time scale: A template for improved rock-based subdivision of pre-Cryogenian time" + } } diff --git a/tests/stubdata/output/crossref_preprint_10.31223-X5WD2C.json b/tests/stubdata/output/crossref_preprint_10.31223-X5WD2C.json index c3c708f..a7d0214 100644 --- a/tests/stubdata/output/crossref_preprint_10.31223-X5WD2C.json +++ b/tests/stubdata/output/crossref_preprint_10.31223-X5WD2C.json @@ -1,74 +1,74 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2022-04-17" - }, - "publication": { - "pubYear": "2022" - }, - "persistentIDs": [ - { - "DOI": "10.31223/X5WD2C" - } - ], "authors": [ { "name": { - "surname": "Halamka", - "given_name": "Toby" + "given_name": "Toby", + "surname": "Halamka" } }, { "name": { - "surname": "Raberg", - "given_name": "Jonathan" + "given_name": "Jonathan", + "surname": "Raberg" } }, { "name": { - "surname": "McFarlin", - "given_name": "Jamie" + "given_name": "Jamie", + "surname": "McFarlin" } }, { "name": { - "surname": "Younkin", - "given_name": "Adam" + "given_name": "Adam", + "surname": "Younkin" } }, { "name": { - "surname": "Mulligan", - "given_name": "Christopher" + "given_name": "Christopher", + "surname": "Mulligan" } }, { "name": { - "surname": "Liu", - "given_name": "Xiao-Lei" + "given_name": "Xiao-Lei", + "surname": "Liu" } }, { "name": { - "surname": "Kopf", - "given_name": "Sebastian" + "given_name": "Sebastian", + "surname": "Kopf" } } ], - "title": { - "textEnglish": "Production of diverse brGDGTs by Acidobacterium Solibacter usitatus in response to temperature, pH, and O2 provides a culturing perspective on brGDGT paleoproxies and biosynthesis" - }, "esources": [ { - "source": "pub_html", - "location": "http://eartharxiv.org/repository/view/3263/" + "location": "http://eartharxiv.org/repository/view/3263/", + "source": "pub_html" } - ] + ], + "persistentIDs": [ + { + "DOI": "10.31223/X5WD2C" + } + ], + "pubDate": { + "electrDate": "2022-04-17" + }, + "publication": { + "pubYear": "2022" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "title": { + "textEnglish": "Production of diverse brGDGTs by Acidobacterium Solibacter usitatus in response to temperature, pH, and O2 provides a culturing perspective on brGDGT paleoproxies and biosynthesis" + } } diff --git a/tests/stubdata/output/datacite_schema3.1_example-full.json b/tests/stubdata/output/datacite_schema3.1_example-full.json index 63451cd..279eaaf 100644 --- a/tests/stubdata/output/datacite_schema3.1_example-full.json +++ b/tests/stubdata/output/datacite_schema3.1_example-full.json @@ -1,53 +1,9 @@ { - 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}, "affiliation": [ { "affPubRaw": "DataCite" @@ -55,18 +11,29 @@ ], "attrib": { "orcid": "0000-0001-5000-0007" + }, + "name": { + "given_name": "Elizabeth", + "pubraw": "Miller, Elizabeth", + "surname": "Miller" } } ], + "doctype": "software", + "keywords": [ + { + "keyString": "000 computer science", + "keySystem": "datacite" + } + ], + "openAccess": { + "license": "CC0 1.0 Universal", + "licenseURL": "http://creativecommons.org/publicdomain/zero/1.0/", + "open": true + }, "otherContributor": [ { - "role": "ProjectLeader", "contrib": { - "name": { - "surname": "Starr", - "given_name": "Joan", - "pubraw": "Starr, Joan" - }, "affiliation": [ { "affPubRaw": "California Digital Library" @@ -74,29 +41,62 @@ ], "attrib": { "orcid": "0000-0002-7285-027X" + }, + "name": { + "given_name": "Joan", + "pubraw": "Starr, Joan", + "surname": "Starr" } - } + }, + "role": "ProjectLeader" } ], - "title": { - "textEnglish": "Full DataCite XML Example" + "persistentIDs": [ + { + "DOI": "10.5072/example-full" + } + ], + "pubDate": { + "electrDate": "2014", + "otherDate": [ + { + "otherDateType": "Updated", + "otherDateValue": "2014-10-17" + } + ] }, - "subtitle": { - "textEnglish": "Demonstration of DataCite Properties." + "publication": { + "pubYear": "2014", + "publisher": "DataCite" }, - "abstract": { - "textEnglish": "XML example of all DataCite Metadata Schema v3.1 properties." + "publisherIDs": [ + { + "Identifier": "http://schema.datacite.org/schema/meta/kernel-3.1/example/datacite-example-full-v3.1.xml", + "attribute": "URL" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, - "doctype": "software", - "keywords": [ + "relatedTo": [ { - "keyString": "000 computer science", - "keySystem": "datacite" + "relatedDocID": "http://data.datacite.org/application/citeproc+json/10.5072/example-full", + "relationship": "related" + }, + { + "relatedDocID": "arXiv:0706.0001", + "relationship": "related" } ], - "openAccess": { - "open": true, - "license": "CC0 1.0 Universal", - "licenseURL": "http://creativecommons.org/publicdomain/zero/1.0/" + "subtitle": { + "textEnglish": "Demonstration of DataCite Properties." + }, + "title": { + "textEnglish": "Full DataCite XML Example" } } diff --git a/tests/stubdata/output/datacite_schema4.1_example-full.json b/tests/stubdata/output/datacite_schema4.1_example-full.json index aa10e03..e1cc2f4 100644 --- a/tests/stubdata/output/datacite_schema4.1_example-full.json +++ b/tests/stubdata/output/datacite_schema4.1_example-full.json @@ -1,52 +1,9 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "relatedTo": [ - { - "relationship": "related", - "relatedDocID": "https://data.datacite.org/application/citeproc+json/10.5072/example-full" - }, - { - "relationship": "related", - "relatedDocID": "arXiv:0706.0001" - } - ], - "pubDate": { - "electrDate": "2014", - "otherDate": [ - { - "otherDateType": "Updated", - "otherDateValue": "2017-09-13" - } - ] - }, - "publication": { - "publisher": "DataCite", - "pubYear": "2014" + "abstract": { + "textEnglish": "XML example of all DataCite Metadata Schema v4.1 properties." }, - "persistentIDs": [ - { - "DOI": "10.5072/example-full" - } - ], - "publisherIDs": [ - { - "attribute": "URL", - "Identifier": "https://schema.datacite.org/meta/kernel-4.1/example/datacite-example-full-v4.1.xml" - } - ], "authors": [ { - "name": { - "surname": "Miller", - "given_name": "Elizabeth" - }, "affiliation": [ { "affPubRaw": "DataCite" @@ -54,17 +11,28 @@ ], "attrib": { "orcid": "0000-0001-5000-0007" + }, + "name": { + "given_name": "Elizabeth", + "surname": "Miller" } } ], + "doctype": "software", + "keywords": [ + { + "keyString": "000 computer science", + "keySystem": "datacite" + } + ], + "openAccess": { + "license": "CC0 1.0 Universal", + "licenseURL": "http://creativecommons.org/publicdomain/zero/1.0/", + "open": true + }, "otherContributor": [ { - "role": "ProjectLeader", "contrib": { - "name": { - "surname": "Starr", - "given_name": "Joan" - }, "affiliation": [ { "affPubRaw": "California Digital Library" @@ -72,29 +40,61 @@ ], "attrib": { "orcid": "0000-0002-7285-027X" + }, + "name": { + "given_name": "Joan", + "surname": "Starr" } - } + }, + "role": "ProjectLeader" } ], - "title": { - "textEnglish": "Full DataCite XML Example" + "persistentIDs": [ + { + "DOI": "10.5072/example-full" + } + ], + "pubDate": { + "electrDate": "2014", + "otherDate": [ + { + "otherDateType": "Updated", + "otherDateValue": "2017-09-13" + } + ] }, - "subtitle": { - "textEnglish": "Demonstration of DataCite Properties." + "publication": { + "pubYear": "2014", + "publisher": "DataCite" }, - "abstract": { - "textEnglish": "XML example of all DataCite Metadata Schema v4.1 properties." + "publisherIDs": [ + { + "Identifier": "https://schema.datacite.org/meta/kernel-4.1/example/datacite-example-full-v4.1.xml", + "attribute": "URL" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, - "doctype": "software", - "keywords": [ + "relatedTo": [ { - "keyString": "000 computer science", - "keySystem": "datacite" + "relatedDocID": "https://data.datacite.org/application/citeproc+json/10.5072/example-full", + "relationship": "related" + }, + { + "relatedDocID": "arXiv:0706.0001", + "relationship": "related" } ], - "openAccess": { - "open": true, - "license": "CC0 1.0 Universal", - "licenseURL": "http://creativecommons.org/publicdomain/zero/1.0/" + "subtitle": { + "textEnglish": "Demonstration of DataCite Properties." + }, + "title": { + "textEnglish": "Full DataCite XML Example" } } diff --git a/tests/stubdata/output/datacite_schema4.1_example-software.json b/tests/stubdata/output/datacite_schema4.1_example-software.json index b65784b..d68cb84 100644 --- a/tests/stubdata/output/datacite_schema4.1_example-software.json +++ b/tests/stubdata/output/datacite_schema4.1_example-software.json @@ -1,117 +1,61 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "relatedTo": [ - { - "relationship": "updated", - "relatedDocID": "doi:10.5072/example-software-1.0" - }, - { - "relationship": "related", - "relatedDocID": "doi:10.5072/example-software-repository" - } - ], - "pubDate": { - "electrDate": "2017", - "otherDate": [ - { - "otherDateType": "Issued", - "otherDateValue": "2017-05-08" - }, - { - "otherDateType": "Available", - "otherDateValue": "2017-05-08" - } - ] - }, - "publication": { - "publisher": "Apollo - University of Cambridge Repository", - "pubYear": "2017" + "abstract": { + "textEnglish": "Set of scripts used to process direct infusion mass spectrometry data as described in the associated paper" }, - "persistentIDs": [ - { - "DOI": "10.5072/example-software-2.0" - } - ], "authors": [ { - "name": { - "surname": "Zielinski", - "given_name": "AT", - "pubraw": "Zielinski, AT" - }, "attrib": { "orcid": "0000-0002-2997-2175" + }, + "name": { + "given_name": "AT", + "pubraw": "Zielinski, AT", + "surname": "Zielinski" } }, { "name": { - "surname": "Kalberer", "given_name": "M", - "pubraw": "Kalberer, M" + "pubraw": "Kalberer, M", + "surname": "Kalberer" } }, { "name": { - "surname": "Bortolini", "given_name": "C", - "pubraw": "Bortolini, C" + "pubraw": "Bortolini, C", + "surname": "Bortolini" } }, { "name": { - "surname": "Giorio", "given_name": "C", - "pubraw": "Giorio, C" + "pubraw": "Giorio, C", + "surname": "Giorio" } }, { "name": { - "surname": "Fuller", "given_name": "SJ", - "pubraw": "Fuller, SJ" + "pubraw": "Fuller, SJ", + "surname": "Fuller" } }, { "name": { - "surname": "Kourtchev", "given_name": "I", - "pubraw": "Kourtchev, I" + "pubraw": "Kourtchev, I", + "surname": "Kourtchev" } }, { "name": { - "surname": "Popoola", "given_name": "O", - "pubraw": "Popoola, O" + "pubraw": "Popoola, O", + "surname": "Popoola" } } ], - "otherContributor": [ - { - "role": "HostingInstitution", - "contrib": { - "name": { - "surname": "Cambridge Repository", - "given_name": "Apollo", - "middle_name": "- University of", - "pubraw": "Apollo - University of Cambridge Repository" - } - } - } - ], - "title": { - "textEnglish": "Code supporting \"A new processing scheme for ultra-high resolution direct infusion mass spectrometry data\"" - }, - "abstract": { - "textEnglish": "Set of scripts used to process direct infusion mass spectrometry data as described in the associated paper" - }, "doctype": "software", "keywords": [ { @@ -140,8 +84,64 @@ } ], "openAccess": { - "open": true, "license": "GNU General Public License version 3", - "licenseURL": "https://opensource.org/licenses/GPL-3.0" + "licenseURL": "https://opensource.org/licenses/GPL-3.0", + "open": true + }, + "otherContributor": [ + { + "contrib": { + "name": { + "given_name": "Apollo", + "middle_name": "- University of", + "pubraw": "Apollo - University of Cambridge Repository", + "surname": "Cambridge Repository" + } + }, + "role": "HostingInstitution" + } + ], + "persistentIDs": [ + { + "DOI": "10.5072/example-software-2.0" + } + ], + "pubDate": { + "electrDate": "2017", + "otherDate": [ + { + "otherDateType": "Issued", + "otherDateValue": "2017-05-08" + }, + { + "otherDateType": "Available", + "otherDateValue": "2017-05-08" + } + ] + }, + "publication": { + "pubYear": "2017", + "publisher": "Apollo - University of Cambridge Repository" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "relatedTo": [ + { + "relatedDocID": "doi:10.5072/example-software-1.0", + "relationship": "updated" + }, + { + "relatedDocID": "doi:10.5072/example-software-repository", + "relationship": "related" + } + ], + "title": { + "textEnglish": "Code supporting \"A new processing scheme for ultra-high resolution direct infusion mass spectrometry data\"" } } diff --git a/tests/stubdata/output/datacite_schema4_example-habanero-pdsdataset.json b/tests/stubdata/output/datacite_schema4_example-habanero-pdsdataset.json index 3acddee..365fa7b 100644 --- a/tests/stubdata/output/datacite_schema4_example-habanero-pdsdataset.json +++ b/tests/stubdata/output/datacite_schema4_example-habanero-pdsdataset.json @@ -1,104 +1,104 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "relatedTo": [ - { - "relationship": "supplement", - "relatedDocID": "10.1016/j.icarus.2009.02.005" - } - ], - "pubDate": { - "electrDate": "2020", - "otherDate": [ - { - "otherDateType": "Available", - "otherDateValue": "2020-08-14" - } - ] - }, - "publication": { - "publisher": "NASA Planetary Data System ", - "pubYear": "2020" + "abstract": { + "textEnglish": "The Bus-DeMeo asteroid taxonomy classification system, described in DeMeo et al. (2009), is based on reflectance spectrum characteristics for 371 asteroids measured over the wavelength 0.45 to 2.45 microns. This system of 24 classes is constructed using principal component analysis, following most closely the visible wavelength taxonomy of Bus (1999), which itself builds upon the system of Tholen (1984). Nearly all of the Bus taxonomy classes are preserved, with one new class (Sv) defined. This data set includes a table of classifications in the Bus-DeMeo system for the 371 asteroids upon which the system is based. It also includes mean spectra for each of the classes." }, - "persistentIDs": [ - { - "DOI": "10.26033/089P-C283" - } - ], - "publisherIDs": [ - { - "attribute": "PDS4 Bundle LIDVID", - "Identifier": "urn:nasa:pds:ast.bus-demeo.taxonomy::1.0" - } - ], "authors": [ { - "name": { - "surname": "DeMeo", - "given_name": "Francesca" - }, "attrib": { "orcid": "0000-0002-8397-4219" + }, + "name": { + "given_name": "Francesca", + "surname": "DeMeo" } }, { - "name": { - "surname": "Binzel", - "given_name": "Richard P." - }, "attrib": { "orcid": "0000-0002-9995-7341" + }, + "name": { + "given_name": "Richard P.", + "surname": "Binzel" } }, { - "name": { - "surname": "Slivan", - "given_name": "Stephen M." - }, "attrib": { "orcid": "0000-0003-3291-8708" + }, + "name": { + "given_name": "Stephen M.", + "surname": "Slivan" } }, { - "name": { - "surname": "Bus", - "given_name": "Schelte J." - }, "attrib": { "orcid": "0000-0003-4191-6536" + }, + "name": { + "given_name": "Schelte J.", + "surname": "Bus" } } ], + "doctype": "misc", + "keywords": [ + { + "keyID": "72", + "keyString": "Asteroids", + "keySystem": "UAT" + } + ], "otherContributor": [ { - "role": "DataCurator", "contrib": { "name": { - "surname": "Small Bodies Node", "given_name": "PDS", - "pubraw": "PDS Small Bodies Node" + "pubraw": "PDS Small Bodies Node", + "surname": "Small Bodies Node" } - } + }, + "role": "DataCurator" } ], - "title": { - "textEnglish": "Bus-DeMeo Asteroid Taxonomy Bundle V1.0" + "persistentIDs": [ + { + "DOI": "10.26033/089P-C283" + } + ], + "pubDate": { + "electrDate": "2020", + "otherDate": [ + { + "otherDateType": "Available", + "otherDateValue": "2020-08-14" + } + ] }, - "abstract": { - "textEnglish": "The Bus-DeMeo asteroid taxonomy classification system, described in DeMeo et al. (2009), is based on reflectance spectrum characteristics for 371 asteroids measured over the wavelength 0.45 to 2.45 microns. This system of 24 classes is constructed using principal component analysis, following most closely the visible wavelength taxonomy of Bus (1999), which itself builds upon the system of Tholen (1984). Nearly all of the Bus taxonomy classes are preserved, with one new class (Sv) defined. This data set includes a table of classifications in the Bus-DeMeo system for the 371 asteroids upon which the system is based. It also includes mean spectra for each of the classes." + "publication": { + "pubYear": "2020", + "publisher": "NASA Planetary Data System " }, - "doctype": "misc", - "keywords": [ + "publisherIDs": [ { - "keyString": "Asteroids", - "keySystem": "UAT", - "keyID": "72" + "Identifier": "urn:nasa:pds:ast.bus-demeo.taxonomy::1.0", + "attribute": "PDS4 Bundle LIDVID" } - ] + ], + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "relatedTo": [ + { + "relatedDocID": "10.1016/j.icarus.2009.02.005", + "relationship": "supplement" + } + ], + "title": { + "textEnglish": "Bus-DeMeo Asteroid Taxonomy Bundle V1.0" + } } diff --git a/tests/stubdata/output/els_missing_keywords_tag.json b/tests/stubdata/output/els_missing_keywords_tag.json index d95db44..11b97f0 100644 --- a/tests/stubdata/output/els_missing_keywords_tag.json +++ b/tests/stubdata/output/els_missing_keywords_tag.json @@ -1,6 +1,6 @@ { "abstract": { - "textEnglish": "In this issue of Chem, Nagib and co-workers report an operationally simple approach for direct C–H halogenation of arenes and (hetero)arenes through in situ activation of commercially available PhI(OAc)2. The resulting non-symmetrical iodanes offer chemists new tools for the mild halogenation of arene scaffolds with exquisite selectivity and tunability." + "textEnglish": "In this issue of Chem, Nagib and co-workers report an operationally simple approach for direct C\u2013H halogenation of arenes and (hetero)arenes through in situ activation of commercially available PhI(OAc)2. The resulting non-symmetrical iodanes offer chemists new tools for the mild halogenation of arene scaffolds with exquisite selectivity and tunability." }, "authors": [ { diff --git a/tests/stubdata/output/jats_a+a_multiparagraph_abstract.json b/tests/stubdata/output/jats_a+a_multiparagraph_abstract.json index d5d6691..d9399ea 100644 --- a/tests/stubdata/output/jats_a+a_multiparagraph_abstract.json +++ b/tests/stubdata/output/jats_a+a_multiparagraph_abstract.json @@ -1,314 +1,367 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2021-12-20" - ], - "acceptedDate": "2022-11-12" - }, - "pubDate": { - "electrDate": "2023-01-27", - "printDate": "2023-02-00" - }, - "publication": { - "pubName": "Astronomy & Astrophysics", - "publisher": "EDP Sciences", - "issueNum": "None", - "volumeNum": "670", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "0004-6361" - }, - { - "pubtype": "epub", - "issnString": "1432-0746" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1051/0004-6361/202142959" - } - ], - "publisherIDs": [ - { - "attribute": "publisher-id", - "Identifier": "aa42959-21" - }, - { - "attribute": "other", - "Identifier": "2023A%26A...670A..13L" - } - ], - "pagination": { - "pageCount": "13", - "electronicID": "A13" + "abstract": { + "textEnglish": "Context. V838 Monocerotis is a peculiar binary that underwent an immense stellar explosion in 2002, leaving behind an expanding cool supergiant and a hot B3V companion. Five years after the outburst, the B3V companion disappeared from view, and has not returned to its original state.\nAims. We investigate the changes in the light curve and spectral features to explain the behaviour of V838 Mon during the current long-lasting minimum.\nMethods. A monitoring campaign has been performed over the past 13 years with the Nordic Optical Telescope to obtain optical photometric and spectroscopic data. The datasets are used to analyse the temporal evolution of the spectral features and the spectral energy distribution, and to characterise the object.\nResults. Our photometric data show a steady brightening in all bands over the past 13 years, which is particularly prominent in the blue. This rise is also reflected in the spectra, showing a gradual relative increase in the continuum flux at shorter wavelengths. In addition, a slow brightening of the H\u03b1 emission line starting in 2015 was detected. These changes might imply that the B3V companion is slowly reappearing. During the same time interval, our analysis reveals a considerable change in the observed colours of the object along with a steady decrease in the strength and width of molecular absorption bands in our low-resolution spectra. These changes suggest a rising temperature of the cool supergiant along with a weakening of its wind, most likely combined with a slow recovery of the secondary due to the evaporation of the dust and accretion of the material from the shell in which the hot companion is embedded. From our medium-resolution spectra, we find that the heliocentric radial velocity of the atomic absorption line of Ti I 6556.06 \u00c5 has been stable for more than a decade. We propose that Ti I lines are tracing the velocity of the red supergiant in V838 Mon, and do not represent the infalling matter as previously stated. \u22c6 Full Tables 2 and 4 and spectra (FITS files) are only available at the CDS via anonymous ftp to cdsarc.cds.unistra.fr (130.79.128.5) or via https://cdsarc.cds.unistra.fr/viz-bin/cat/J/A+A/670/A13" }, "authors": [ { - "name": { - "surname": "Liimets", - "given_name": "T." - }, "affiliation": [ { - "affPubRaw": "Astronomical Institute, Czech Academy of Sciences, Fri\u010dova 298, 25165 Ond\u0159ejov, Czech Republic", - "affPubID": "AFF1" + "affPubID": "AFF1", + "affPubRaw": "Astronomical Institute, Czech Academy of Sciences, Fri\u010dova 298, 25165 Ond\u0159ejov, Czech Republic" }, { - "affPubRaw": "Tartu Observatory, University of Tartu, Observatooriumi 1, 61602 T\u00f5ravere, Estonia", - "affPubID": "AFF2" + "affPubID": "AFF2", + "affPubRaw": "Tartu Observatory, University of Tartu, Observatooriumi 1, 61602 T\u00f5ravere, Estonia" } ], "attrib": { "orcid": "0000-0003-2196-9091" + }, + "name": { + "given_name": "T.", + "surname": "Liimets" } }, { - "name": { - "surname": "Kolka", - "given_name": "I." - }, "affiliation": [ { - "affPubRaw": "Tartu Observatory, University of Tartu, Observatooriumi 1, 61602 T\u00f5ravere, Estonia", - "affPubID": "AFF2" + "affPubID": "AFF2", + "affPubRaw": "Tartu Observatory, University of Tartu, Observatooriumi 1, 61602 T\u00f5ravere, Estonia" } - ] + ], + "name": { + "given_name": "I.", + "surname": "Kolka" + } }, { - "name": { - "surname": "Kraus", - "given_name": "M." - }, "affiliation": [ { - "affPubRaw": "Astronomical Institute, Czech Academy of Sciences, Fri\u010dova 298, 25165 Ond\u0159ejov, Czech Republic", - "affPubID": "AFF1" + "affPubID": "AFF1", + "affPubRaw": "Astronomical Institute, Czech Academy of Sciences, Fri\u010dova 298, 25165 Ond\u0159ejov, Czech Republic" } ], "attrib": { "orcid": "0000-0002-4502-6330" + }, + "name": { + "given_name": "M.", + "surname": "Kraus" } }, { - "name": { - "surname": "Eenm\u00e4e", - "given_name": "T." - }, "affiliation": [ { - "affPubRaw": "Tartu Observatory, University of Tartu, Observatooriumi 1, 61602 T\u00f5ravere, Estonia", - "affPubID": "AFF2" + "affPubID": "AFF2", + "affPubRaw": "Tartu Observatory, University of Tartu, Observatooriumi 1, 61602 T\u00f5ravere, Estonia" } - ] + ], + "name": { + "given_name": "T.", + "surname": "Eenm\u00e4e" + } }, { - "name": { - "surname": "Tuvikene", - "given_name": "T." - }, "affiliation": [ { - "affPubRaw": "Tartu Observatory, University of Tartu, Observatooriumi 1, 61602 T\u00f5ravere, Estonia", - "affPubID": "AFF2" + "affPubID": "AFF2", + "affPubRaw": "Tartu Observatory, University of Tartu, Observatooriumi 1, 61602 T\u00f5ravere, Estonia" } - ] + ], + "name": { + "given_name": "T.", + "surname": "Tuvikene" + } }, { - "name": { - "surname": "Augusteijn", - "given_name": "T." - }, "affiliation": [ { - "affPubRaw": "Nordic Optical Telescope, Rambla Jos\u00e9 Ana Fern\u00e1ndez, P\u00e9rez 7, 38711 Bre\u00f1a Baja, Spain", - "affPubID": "AFF3" + "affPubID": "AFF3", + "affPubRaw": "Nordic Optical Telescope, Rambla Jos\u00e9 Ana Fern\u00e1ndez, P\u00e9rez 7, 38711 Bre\u00f1a Baja, Spain" }, { - "affPubRaw": "Department of Physics and Astronomy, Aarhus University, Munkegade 120, 8000 Aarhus C, Denmark", - "affPubID": "AFF4" + "affPubID": "AFF4", + "affPubRaw": "Department of Physics and Astronomy, Aarhus University, Munkegade 120, 8000 Aarhus C, Denmark" } - ] + ], + "name": { + "given_name": "T.", + "surname": "Augusteijn" + } }, { - "name": { - "surname": "Antunes Amaral", - "given_name": "L." - }, "affiliation": [ { - "affPubRaw": "Instituto de F\u00edsica y Astronom\u00eda, Universidad de Valpara\u00edso, Gran Breta\u00f1a 1111, Playa Ancha, Valpara\u00edso 2360102, Chile", - "affPubID": "AFF5" + "affPubID": "AFF5", + "affPubRaw": "Instituto de F\u00edsica y Astronom\u00eda, Universidad de Valpara\u00edso, Gran Breta\u00f1a 1111, Playa Ancha, Valpara\u00edso 2360102, Chile" } - ] + ], + "name": { + "given_name": "L.", + "surname": "Antunes Amaral" + } }, { - "name": { - "surname": "Djupvik", - "given_name": "A. A." - }, "affiliation": [ { - "affPubRaw": "Nordic Optical Telescope, Rambla Jos\u00e9 Ana Fern\u00e1ndez, P\u00e9rez 7, 38711 Bre\u00f1a Baja, Spain", - "affPubID": "AFF3" + "affPubID": "AFF3", + "affPubRaw": "Nordic Optical Telescope, Rambla Jos\u00e9 Ana Fern\u00e1ndez, P\u00e9rez 7, 38711 Bre\u00f1a Baja, Spain" }, { - "affPubRaw": "Department of Physics and Astronomy, Aarhus University, Munkegade 120, 8000 Aarhus C, Denmark", - "affPubID": "AFF4" + "affPubID": "AFF4", + "affPubRaw": "Department of Physics and Astronomy, Aarhus University, Munkegade 120, 8000 Aarhus C, Denmark" } ], "attrib": { "orcid": "0000-0001-6316-9880" + }, + "name": { + "given_name": "A. A.", + "surname": "Djupvik" } }, { - "name": { - "surname": "Telting", - "given_name": "J. H." - }, "affiliation": [ { - "affPubRaw": "Nordic Optical Telescope, Rambla Jos\u00e9 Ana Fern\u00e1ndez, P\u00e9rez 7, 38711 Bre\u00f1a Baja, Spain", - "affPubID": "AFF3" + "affPubID": "AFF3", + "affPubRaw": "Nordic Optical Telescope, Rambla Jos\u00e9 Ana Fern\u00e1ndez, P\u00e9rez 7, 38711 Bre\u00f1a Baja, Spain" }, { - "affPubRaw": "Department of Physics and Astronomy, Aarhus University, Munkegade 120, 8000 Aarhus C, Denmark", - "affPubID": "AFF4" + "affPubID": "AFF4", + "affPubRaw": "Department of Physics and Astronomy, Aarhus University, Munkegade 120, 8000 Aarhus C, Denmark" } - ] + ], + "name": { + "given_name": "J. H.", + "surname": "Telting" + } }, { - "name": { - "surname": "Deshev", - "given_name": "B." - }, "affiliation": [ { - "affPubRaw": "Astronomical Institute, Czech Academy of Sciences, Fri\u010dova 298, 25165 Ond\u0159ejov, Czech Republic", - "affPubID": "AFF1" + "affPubID": "AFF1", + "affPubRaw": "Astronomical Institute, Czech Academy of Sciences, Fri\u010dova 298, 25165 Ond\u0159ejov, Czech Republic" } - ] + ], + "name": { + "given_name": "B.", + "surname": "Deshev" + } }, { - "name": { - "surname": "Kankare", - "given_name": "E." - }, "affiliation": [ { - "affPubRaw": "Tuorla Observatory, Department of Physics and Astronomy, University of Turku, 20014 Turku, Finland", - "affPubID": "AFF6" + "affPubID": "AFF6", + "affPubRaw": "Tuorla Observatory, Department of Physics and Astronomy, University of Turku, 20014 Turku, Finland" } - ] + ], + "name": { + "given_name": "E.", + "surname": "Kankare" + } }, { - "name": { - "surname": "Kankare", - "given_name": "J." - }, "affiliation": [ { - "affPubRaw": "Astronomical Institute, Czech Academy of Sciences, Fri\u010dova 298, 25165 Ond\u0159ejov, Czech Republic", - "affPubID": "AFF1" + "affPubID": "AFF1", + "affPubRaw": "Astronomical Institute, Czech Academy of Sciences, Fri\u010dova 298, 25165 Ond\u0159ejov, Czech Republic" } - ] + ], + "name": { + "given_name": "J.", + "surname": "Kankare" + } }, { - "name": { - "surname": "Lindberg", - "given_name": "J. E." - }, "affiliation": [ { - "affPubRaw": "Astronomical Institute, Czech Academy of Sciences, Fri\u010dova 298, 25165 Ond\u0159ejov, Czech Republic", - "affPubID": "AFF1" + "affPubID": "AFF1", + "affPubRaw": "Astronomical Institute, Czech Academy of Sciences, Fri\u010dova 298, 25165 Ond\u0159ejov, Czech Republic" } ], "attrib": { "orcid": "0000-0003-3811-4591" + }, + "name": { + "given_name": "J. E.", + "surname": "Lindberg" } }, { - "name": { - "surname": "Amby", - "given_name": "T. M." - }, "affiliation": [ { - "affPubRaw": "Viborg Katedralskole, Gl.Skivevej 2, 8800 Viborg, Denmark", - "affPubID": "AFF7" + "affPubID": "AFF7", + "affPubRaw": "Viborg Katedralskole, Gl.Skivevej 2, 8800 Viborg, Denmark" } - ] + ], + "name": { + "given_name": "T. M.", + "surname": "Amby" + } }, { - "name": { - "surname": "Pursimo", - "given_name": "T." - }, "affiliation": [ { - "affPubRaw": "Nordic Optical Telescope, Rambla Jos\u00e9 Ana Fern\u00e1ndez, P\u00e9rez 7, 38711 Bre\u00f1a Baja, Spain", - "affPubID": "AFF3" + "affPubID": "AFF3", + "affPubRaw": "Nordic Optical Telescope, Rambla Jos\u00e9 Ana Fern\u00e1ndez, P\u00e9rez 7, 38711 Bre\u00f1a Baja, Spain" }, { - "affPubRaw": "Department of Physics and Astronomy, Aarhus University, Munkegade 120, 8000 Aarhus C, Denmark", - "affPubID": "AFF4" + "affPubID": "AFF4", + "affPubRaw": "Department of Physics and Astronomy, Aarhus University, Munkegade 120, 8000 Aarhus C, Denmark" } - ] + ], + "name": { + "given_name": "T.", + "surname": "Pursimo" + } }, { - "name": { - "surname": "Somero", - "given_name": "A." - }, "affiliation": [ { - "affPubRaw": "Tuorla Observatory, Department of Physics and Astronomy, University of Turku, 20014 Turku, Finland", - "affPubID": "AFF6" + "affPubID": "AFF6", + "affPubRaw": "Tuorla Observatory, Department of Physics and Astronomy, University of Turku, 20014 Turku, Finland" } - ] + ], + "name": { + "given_name": "A.", + "surname": "Somero" + } }, { - "name": { - "surname": "Thygesen", - "given_name": "A." - }, "affiliation": [ { - "affPubRaw": "Department of Physics, University of Warwick, Coventry CV4 7AL, UK", - "affPubID": "AFF8" + "affPubID": "AFF8", + "affPubRaw": "Department of Physics, University of Warwick, Coventry CV4 7AL, UK" }, { - "affPubRaw": "Institut d\u2019astrophysique de Paris, CNRS, UMR 7095 & Sorbonne Universit\u00e9s, UPMC Paris 6, 98 Boulevard Arago, 75014 Paris, France", - "affPubID": "AFF9" + "affPubID": "AFF9", + "affPubRaw": "Institut d\u2019astrophysique de Paris, CNRS, UMR 7095 & Sorbonne Universit\u00e9s, UPMC Paris 6, 98 Boulevard Arago, 75014 Paris, France" } - ] + ], + "name": { + "given_name": "A.", + "surname": "Thygesen" + } }, { "name": { - "surname": "Str\u00f8m", - "given_name": "P. A." + "given_name": "P. A.", + "surname": "Str\u00f8m" } } ], - "title": { - "textEnglish": "V838 Mon: A slow waking up of Sleeping Beauty?", - "textNotes": [ - "\u22c6 Full Tables 2 and 4 and spectra (FITS files) are only available at the CDS via anonymous ftp to cdsarc.cds.unistra.fr (130.79.128.5) or via https://cdsarc.cds.unistra.fr/viz-bin/cat/J/A+A/670/A13" + "copyright": { + "statement": "\u00a9 T. Liimets et al. 2023", + "status": true + }, + "editorialHistory": { + "acceptedDate": "2022-11-12", + "receivedDates": [ + "2021-12-20" ] }, - "abstract": { - "textEnglish": "Context. V838 Monocerotis is a peculiar binary that underwent an immense stellar explosion in 2002, leaving behind an expanding cool supergiant and a hot B3V companion. Five years after the outburst, the B3V companion disappeared from view, and has not returned to its original state.\nAims. We investigate the changes in the light curve and spectral features to explain the behaviour of V838 Mon during the current long-lasting minimum.\nMethods. A monitoring campaign has been performed over the past 13 years with the Nordic Optical Telescope to obtain optical photometric and spectroscopic data. The datasets are used to analyse the temporal evolution of the spectral features and the spectral energy distribution, and to characterise the object.\nResults. Our photometric data show a steady brightening in all bands over the past 13 years, which is particularly prominent in the blue. This rise is also reflected in the spectra, showing a gradual relative increase in the continuum flux at shorter wavelengths. In addition, a slow brightening of the H\u03b1 emission line starting in 2015 was detected. These changes might imply that the B3V companion is slowly reappearing. During the same time interval, our analysis reveals a considerable change in the observed colours of the object along with a steady decrease in the strength and width of molecular absorption bands in our low-resolution spectra. These changes suggest a rising temperature of the cool supergiant along with a weakening of its wind, most likely combined with a slow recovery of the secondary due to the evaporation of the dust and accretion of the material from the shell in which the hot companion is embedded. From our medium-resolution spectra, we find that the heliocentric radial velocity of the atomic absorption line of Ti I 6556.06 \u00c5 has been stable for more than a decade. We propose that Ti I lines are tracing the velocity of the red supergiant in V838 Mon, and do not represent the infalling matter as previously stated. \u22c6 Full Tables 2 and 4 and spectra (FITS files) are only available at the CDS via anonymous ftp to cdsarc.cds.unistra.fr (130.79.128.5) or via https://cdsarc.cds.unistra.fr/viz-bin/cat/J/A+A/670/A13" + "esources": [ + { + "location": "https://www.aanda.org/articles/aa/full_html/2023/02/aa42959-21/aa42959-21.html", + "source": "pub_html" + }, + { + "location": "https://www.aanda.org/articles/aa/pdf/2023/02/aa42959-21.pdf", + "source": "pub_pdf" + } + ], + "funding": [ + { + "agencyid": { + "idvalue": "Czech Science Foundation" + }, + "awardnumber": "20-00150S" + }, + { + "agencyid": { + "idvalue": "European Union\u2019s Framework Programme for Research and Innovation Horizon 2020" + }, + "awardnumber": "823734" + } + ], + "keywords": [ + { + "keyString": "stars: individual: V838 Mon", + "keySystem": "misc" + }, + { + "keyString": "stars: evolution", + "keySystem": "misc" + }, + { + "keyString": "stars: peculiar", + "keySystem": "misc" + }, + { + "keyString": "stars: mass-loss", + "keySystem": "misc" + }, + { + "keyString": "techniques: photometric", + "keySystem": "misc" + }, + { + "keyString": "techniques: spectroscopic", + "keySystem": "misc" + } + ], + "openAccess": { + "license": "Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.", + "licenseURL": "https://www.edpsciences.org", + "open": true + }, + "pagination": { + "electronicID": "A13", + "pageCount": "13" + }, + "persistentIDs": [ + { + "DOI": "10.1051/0004-6361/202142959" + } + ], + "pubDate": { + "electrDate": "2023-01-27", + "printDate": "2023-02-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "0004-6361", + "pubtype": "ppub" + }, + { + "issnString": "1432-0746", + "pubtype": "epub" + } + ], + "issueNum": "None", + "pubName": "Astronomy & Astrophysics", + "pubYear": "2023", + "publisher": "EDP Sciences", + "volumeNum": "670" + }, + "publisherIDs": [ + { + "Identifier": "aa42959-21", + "attribute": "publisher-id" + }, + { + "Identifier": "2023A%26A...670A..13L", + "attribute": "other" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " Af\u015far, M., & Bond, H. E. 2007, AJ, 133, 387 ", @@ -367,63 +420,10 @@ " Woodward, C. E., Evans, A., Banerjee, D. P. K., et al. 2021, AJ, 162, 183 ", " Worthey, G., & Lee, H.-C. 2011, A&AS, 193, 1 " ], - "esources": [ - { - "source": "pub_html", - "location": "https://www.aanda.org/articles/aa/full_html/2023/02/aa42959-21/aa42959-21.html" - }, - { - "source": "pub_pdf", - "location": "https://www.aanda.org/articles/aa/pdf/2023/02/aa42959-21.pdf" - } - ], - "keywords": [ - { - "keyString": "stars: individual: V838 Mon", - "keySystem": "misc" - }, - { - "keyString": "stars: evolution", - "keySystem": "misc" - }, - { - "keyString": "stars: peculiar", - "keySystem": "misc" - }, - { - "keyString": "stars: mass-loss", - "keySystem": "misc" - }, - { - "keyString": "techniques: photometric", - "keySystem": "misc" - }, - { - "keyString": "techniques: spectroscopic", - "keySystem": "misc" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 T. Liimets et al. 2023" - }, - "openAccess": { - "open": true, - "license": "Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.", - "licenseURL": "https://www.edpsciences.org" - }, - "funding": [ - { - "agencyid": { - "idvalue": "Czech Science Foundation" - }, - "awardnumber": "20-00150S" - }, - { - "agencyid": { - "idvalue": "European Union\u2019s Framework Programme for Research and Innovation Horizon 2020" - }, - "awardnumber": "823734" - } - ] + "title": { + "textEnglish": "V838 Mon: A slow waking up of Sleeping Beauty?", + "textNotes": [ + "\u22c6 Full Tables 2 and 4 and spectra (FITS files) are only available at the CDS via anonymous ftp to cdsarc.cds.unistra.fr (130.79.128.5) or via https://cdsarc.cds.unistra.fr/viz-bin/cat/J/A+A/670/A13" + ] + } } diff --git a/tests/stubdata/output/jats_a+a_subtitle.json b/tests/stubdata/output/jats_a+a_subtitle.json index a7a1f0d..77b545f 100644 --- a/tests/stubdata/output/jats_a+a_subtitle.json +++ b/tests/stubdata/output/jats_a+a_subtitle.json @@ -1,664 +1,704 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2022-06-07" - ], - "acceptedDate": "2022-11-28" - }, - "pubDate": { - "electrDate": "2023-03-00" - }, - "publication": { - "pubName": "Astronomy & Astrophysics", - "publisher": "EDP Sciences", - "issueNum": "None", - "volumeNum": "671", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "0004-6361" - }, - { - "pubtype": "epub", - "issnString": "1432-0746" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1051/0004-6361/202244205" - } - ], - "publisherIDs": [ - { - "attribute": "publisher-id", - "Identifier": "aa44205-22" - } - ], - "pagination": { - "pageCount": "21", - "electronicID": "A84" + "abstract": { + "textEnglish": "The study of the properties of galaxies in the first billion years after the Big Bang is one of the major topics of current astrophysics. Optical and near-infrared spectroscopy of the afterglows of long gamma-ray bursts (GRBs) provides a powerful diagnostic tool to probe the interstellar medium (ISM) of their host galaxies and foreground absorbers, even up to the highest redshifts. We analyze the VLT/X-shooter afterglow spectrum of GRB 210905A, triggered by the Neil Gehrels Swift Observatory, and detect neutral hydrogen, low-ionization, high-ionization, and fine-structure absorption lines from a complex system at z = 6.3118, which we associate with the GRB host galaxy. We use them to study the ISM properties of the host system, revealing the metallicity, kinematics, and chemical abundance pattern of its gas along the GRB line of sight. We also detect absorption lines from at least two foreground absorbers at z = 5.7390 and z = 2.8296. The total metallicity of the z \u223c 6.3 system is [M/H]tot = \u22121.72 \u00b1 0.13, after correcting for dust depletion and taking \u03b1-element enhancement into account, as suggested by our analysis. This is consistent with the values found for the other two GRBs at z \u223c 6 with spectroscopic data showing metal absorption lines (GRB 050904 and GRB 130606A), and it is at the higher end of the metallicity distribution of quasar damped Lyman-\u03b1 systems (QSO-DLAs) extrapolated to such a high redshift. In addition, we determine the overall amount of dust and dust-to-metal mass ratio (DTM) ([Zn/Fe]fit = 0.33 \u00b1 0.09 and DTM = 0.18 \u00b1 0.03). We find indications of nucleosynthesis due to massive stars and, for some of the components of the gas clouds, we find evidence of peculiar nucleosynthesis, with an overabundance of aluminum (as also found for GRB 130606A). From the analysis of fine-structure lines, we determine distances of several kiloparsecs for the low-ionization gas clouds closest to the GRB. Those are farther distances than usually found for GRB host absorption systems, possibly due to the very high number of ionizing photons produced by the GRB that could ionize the line of sight up to several hundreds of parsecs. Using the HST/F140W image of the GRB field, we show the GRB host galaxy (with a possible afterglow contamination) as well as multiple objects within 2\u2033 from the GRB position. We discuss the galaxy structure and kinematics that could explain our observations, also taking into account a tentative detection of Lyman-\u03b1 emission at z = 6.3449 (\u223c1200 km s\u22121 from the GRB redshift in velocity space), and the observational properties of Lyman-\u03b1 emitters at very high redshift. This study shows the amazing potential of GRBs to access detailed information on the properties (metal enrichment, gas kinematic, dust content, nucleosynthesis...) of very high-redshift galaxies, independently of the galaxy luminosity. Deep spectroscopic observations with VLT/MUSE and JWST will offer the unique possibility of combining the information presented in this paper with the properties of the ionized gas, with the goal of better understanding how galaxies in the reionization era form and evolve." }, "authors": [ { - "name": { - "surname": "Saccardi", - "given_name": "A." - }, "affiliation": [ { - "affPubRaw": "GEPI, Observatoire de Paris, Universit\u00e9 PSL, CNRS, 5 place Jules Janssen, 92190 Meudon, France", - "affPubID": "AFF1" + "affPubID": "AFF1", + "affPubRaw": "GEPI, Observatoire de Paris, Universit\u00e9 PSL, CNRS, 5 place Jules Janssen, 92190 Meudon, France" } ], "attrib": { "orcid": "0000-0002-6950-4587" + }, + "name": { + "given_name": "A.", + "surname": "Saccardi" } }, { - "name": { - "surname": "Vergani", - "given_name": "S. D." - }, "affiliation": [ { - "affPubRaw": "GEPI, Observatoire de Paris, Universit\u00e9 PSL, CNRS, 5 place Jules Janssen, 92190 Meudon, France", - "affPubID": "AFF1" + "affPubID": "AFF1", + "affPubRaw": "GEPI, Observatoire de Paris, Universit\u00e9 PSL, CNRS, 5 place Jules Janssen, 92190 Meudon, France" }, { - "affPubRaw": "INAF \u2013 Osservatorio Astronomico di Brera, Via E. Bianchi 46, 23807 Merate, LC, Italy", - "affPubID": "AFF2" + "affPubID": "AFF2", + "affPubRaw": "INAF \u2013 Osservatorio Astronomico di Brera, Via E. Bianchi 46, 23807 Merate, LC, Italy" }, { - "affPubRaw": "Institut d\u2019Astrophysique de Paris, UMR 7095, CNRS-SU, 98 bis boulevard Arago, 75014 Paris, France", - "affPubID": "AFF3" + "affPubID": "AFF3", + "affPubRaw": "Institut d\u2019Astrophysique de Paris, UMR 7095, CNRS-SU, 98 bis boulevard Arago, 75014 Paris, France" } ], "attrib": { "orcid": "0000-0001-9398-4907" + }, + "name": { + "given_name": "S. D.", + "surname": "Vergani" } }, { - "name": { - "surname": "De Cia", - "given_name": "A." - }, "affiliation": [ { - "affPubRaw": "Department of Astronomy, University of Geneva, Chemin Pegasi 51, 1290 Versoix, Switzerland", - "affPubID": "AFF4" + "affPubID": "AFF4", + "affPubRaw": "Department of Astronomy, University of Geneva, Chemin Pegasi 51, 1290 Versoix, Switzerland" } ], "attrib": { "orcid": "0000-0003-2082-1626" + }, + "name": { + "given_name": "A.", + "surname": "De Cia" } }, { - "name": { - "surname": "D\u2019Elia", - "given_name": "V." - }, "affiliation": [ { - "affPubRaw": "Space Science Data Center (SSDC) \u2013 Agenzia Spaziale Italiana (ASI), 00133 Roma, Italy", - "affPubID": "AFF5" + "affPubID": "AFF5", + "affPubRaw": "Space Science Data Center (SSDC) \u2013 Agenzia Spaziale Italiana (ASI), 00133 Roma, Italy" }, { - "affPubRaw": "INAF \u2013 Osservatorio Astronomico di Roma, Via Frascati 33, 00040 Monte Porzio Catone, Italy", - "affPubID": "AFF6" + "affPubID": "AFF6", + "affPubRaw": "INAF \u2013 Osservatorio Astronomico di Roma, Via Frascati 33, 00040 Monte Porzio Catone, Italy" } ], "attrib": { "orcid": "0000-0003-3703-4418" + }, + "name": { + "given_name": "V.", + "surname": "D\u2019Elia" } }, { - "name": { - "surname": "Heintz", - "given_name": "K. E." - }, "affiliation": [ { - "affPubRaw": "Centre for Astrophysics and Cosmology, Science Institute, University of Iceland, Dunhagi 5, 107 Reykjav\u00edk, Iceland", - "affPubID": "AFF7" + "affPubID": "AFF7", + "affPubRaw": "Centre for Astrophysics and Cosmology, Science Institute, University of Iceland, Dunhagi 5, 107 Reykjav\u00edk, Iceland" }, { - "affPubRaw": "Cosmic Dawn Center (DAWN), Copenhagen, Denmark", - "affPubID": "AFF8" + "affPubID": "AFF8", + "affPubRaw": "Cosmic Dawn Center (DAWN), Copenhagen, Denmark" }, { - "affPubRaw": "Niels Bohr Institute, University of Copenhagen, Jagtvej 128, 2200 Copenhagen N, Denmark", - "affPubID": "AFF9" + "affPubID": "AFF9", + "affPubRaw": "Niels Bohr Institute, University of Copenhagen, Jagtvej 128, 2200 Copenhagen N, Denmark" } - ] + ], + "name": { + "given_name": "K. E.", + "surname": "Heintz" + } }, { - "name": { - "surname": "Izzo", - "given_name": "L." - }, "affiliation": [ { - "affPubRaw": "DARK, Niels Bohr Institute, University of Copenhagen, Jagtvej 128, 2200 Copenhagen, Denmark", - "affPubID": "AFF10" + "affPubID": "AFF10", + "affPubRaw": "DARK, Niels Bohr Institute, University of Copenhagen, Jagtvej 128, 2200 Copenhagen, Denmark" } ], "attrib": { "orcid": "0000-0001-9695-8472" + }, + "name": { + "given_name": "L.", + "surname": "Izzo" } }, { - "name": { - "surname": "Palmerio", - "given_name": "J. T." - }, "affiliation": [ { - "affPubRaw": "GEPI, Observatoire de Paris, Universit\u00e9 PSL, CNRS, 5 place Jules Janssen, 92190 Meudon, France", - "affPubID": "AFF1" + "affPubID": "AFF1", + "affPubRaw": "GEPI, Observatoire de Paris, Universit\u00e9 PSL, CNRS, 5 place Jules Janssen, 92190 Meudon, France" } ], "attrib": { "orcid": "0000-0002-9408-1563" + }, + "name": { + "given_name": "J. 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J." - }, "affiliation": [ { - "affPubRaw": "Department of Astrophysics/IMAPP, Radboud University, 6525 AJ, Nijmegen, The Netherlands", - "affPubID": "AFF13" + "affPubID": "AFF13", + "affPubRaw": "Department of Astrophysics/IMAPP, Radboud University, 6525 AJ, Nijmegen, The Netherlands" } - ] + ], + "name": { + "given_name": "A. J.", + "surname": "Levan" + } }, { - "name": { - "surname": "Malesani", - "given_name": "D. B." - }, "affiliation": [ { - "affPubRaw": "Department of Astrophysics/IMAPP, Radboud University, 6525 AJ, Nijmegen, The Netherlands", - "affPubID": "AFF13" + "affPubID": "AFF13", + "affPubRaw": "Department of Astrophysics/IMAPP, Radboud University, 6525 AJ, Nijmegen, The Netherlands" }, { - "affPubRaw": "Cosmic Dawn Center (DAWN), Copenhagen, Denmark", - "affPubID": "AFF8" + "affPubID": "AFF8", + "affPubRaw": "Cosmic Dawn Center (DAWN), Copenhagen, Denmark" }, { - "affPubRaw": "Niels Bohr Institute, University of Copenhagen, Jagtvej 128, 2200 Copenhagen N, Denmark", - "affPubID": "AFF9" + "affPubID": "AFF9", + "affPubRaw": "Niels Bohr Institute, University of Copenhagen, Jagtvej 128, 2200 Copenhagen N, Denmark" } ], "attrib": { "orcid": "0000-0002-7517-326X" + }, + "name": { + "given_name": "D. 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J." - }, "affiliation": [ { - "affPubRaw": "Department of Physics, the George Washington University, 725 21st Street NW, Washington, DC 20052, USA", - "affPubID": "AFF22" + "affPubID": "AFF22", + "affPubRaw": "Department of Physics, the George Washington University, 725 21st Street NW, Washington, DC 20052, USA" }, { - "affPubRaw": "Astronomy, Physics and Statistics Institute of Sciences (APSIS), 725 21st Street NW, Washington, DC 20052, USA", - "affPubID": "AFF24" + "affPubID": "AFF24", + "affPubRaw": "Astronomy, Physics and Statistics Institute of Sciences (APSIS), 725 21st Street NW, Washington, DC 20052, USA" } - ] + ], + "name": { + "given_name": "A. J.", + "surname": "van der Horst" + } }, { - "name": { - "surname": "Jakobsson", - "given_name": "P." - }, "affiliation": [ { - "affPubRaw": "Centre for Astrophysics and Cosmology, Science Institute, University of Iceland, Dunhagi 5, 107 Reykjav\u00edk, Iceland", - "affPubID": "AFF7" + "affPubID": "AFF7", + "affPubRaw": "Centre for Astrophysics and Cosmology, Science Institute, University of Iceland, Dunhagi 5, 107 Reykjav\u00edk, Iceland" } ], "attrib": { "orcid": "0000-0002-9404-5650" + }, + "name": { + "given_name": "P.", + "surname": "Jakobsson" } }, { - "name": { - "surname": "Palazzi", - "given_name": "E." - }, "affiliation": [ { - "affPubRaw": "INAF \u2013 Osservatorio di Astrofisica e Scienza dello Spazio, Via Piero Gobetti 93/3, 40129 Bologna, Italy", - "affPubID": "AFF11" + "affPubID": "AFF11", + "affPubRaw": "INAF \u2013 Osservatorio di Astrofisica e Scienza dello Spazio, Via Piero Gobetti 93/3, 40129 Bologna, Italy" } ], "attrib": { "orcid": "0000-0002-8691-7666" + }, + "name": { + "given_name": "E.", + "surname": "Palazzi" } }, { - "name": { - "surname": "Pugliese", - "given_name": "G." - }, "affiliation": [ { - "affPubRaw": "Anton Pannekoek Institute for Astronomy, University of Amsterdam, Science Park 904, 1098 XH, Amsterdam, The Netherlands", - "affPubID": "AFF25" + "affPubID": "AFF25", + "affPubRaw": "Anton Pannekoek Institute for Astronomy, University of Amsterdam, Science Park 904, 1098 XH, Amsterdam, The Netherlands" }, { - "affPubRaw": "Leiden Observatory, University of Leiden, Niels Bohrweg 2, 2333 CA Leiden, The Netherlands", - "affPubID": "AFF26" + "affPubID": "AFF26", + "affPubRaw": "Leiden Observatory, University of Leiden, Niels Bohrweg 2, 2333 CA Leiden, The Netherlands" } ], "attrib": { "orcid": "0000-0003-3457-9375" + }, + "name": { + "given_name": "G.", + "surname": "Pugliese" } }, { - "name": { - "surname": "Savaglio", - "given_name": "S." - }, "affiliation": [ { - "affPubRaw": "INAF \u2013 Osservatorio di Astrofisica e Scienza dello Spazio, Via Piero Gobetti 93/3, 40129 Bologna, Italy", - "affPubID": "AFF11" + "affPubID": "AFF11", + "affPubRaw": "INAF \u2013 Osservatorio di Astrofisica e Scienza dello Spazio, Via Piero Gobetti 93/3, 40129 Bologna, Italy" }, { - "affPubRaw": "Physics Department, University of Calabria, 87036 Arcavacata di Rende, CS, Italy", - "affPubID": "AFF27" + "affPubID": "AFF27", + "affPubRaw": "Physics Department, University of Calabria, 87036 Arcavacata di Rende, CS, Italy" }, { - "affPubRaw": "INFN \u2013 Laboratori Nazionali di Frascati, Frascati, Italy", - "affPubID": "AFF28" + "affPubID": "AFF28", + "affPubRaw": "INFN \u2013 Laboratori Nazionali di Frascati, Frascati, Italy" } ], "attrib": { "orcid": "0000-0003-2354-3238" + }, + "name": { + "given_name": "S.", + "surname": "Savaglio" } }, { - "name": { - "surname": "Starling", - "given_name": "R. L. C." - }, "affiliation": [ { - "affPubRaw": "School of Physics and Astronomy, University of Leicester, University Road, Leicester LE1 7RH, UK", - "affPubID": "AFF16" + "affPubID": "AFF16", + "affPubRaw": "School of Physics and Astronomy, University of Leicester, University Road, Leicester LE1 7RH, UK" } ], "attrib": { "orcid": "0000-0001-5803-2038" + }, + "name": { + "given_name": "R. L. C.", + "surname": "Starling" } }, { - "name": { - "surname": "Stratta", - "given_name": "G." - }, "affiliation": [ { - "affPubRaw": "INAF \u2013 Osservatorio di Astrofisica e Scienza dello Spazio, Via Piero Gobetti 93/3, 40129 Bologna, Italy", - "affPubID": "AFF11" + "affPubID": "AFF11", + "affPubRaw": "INAF \u2013 Osservatorio di Astrofisica e Scienza dello Spazio, Via Piero Gobetti 93/3, 40129 Bologna, Italy" } ], "attrib": { "orcid": "0000-0003-1055-7980" + }, + "name": { + "given_name": "G.", + "surname": "Stratta" } }, { - "name": { - "surname": "Zafar", - "given_name": "T." - }, "affiliation": [ { - "affPubRaw": "Australian Astronomical Optics, Macquarie University, 105 Delhi Road, North Ryde, NSW 2113, Australia", - "affPubID": "AFF29" + "affPubID": "AFF29", + "affPubRaw": "Australian Astronomical Optics, Macquarie University, 105 Delhi Road, North Ryde, NSW 2113, Australia" } - ] + ], + "name": { + "given_name": "T.", + "surname": "Zafar" + } } ], - "title": { - "textEnglish": "Dissecting the interstellar medium of a z = 6.3 galaxy" + "copyright": { + "statement": "\u00a9 The Authors 2023", + "status": true }, - "subtitle": { - "textEnglish": "X-shooter spectroscopy and HST imaging of the afterglow and environment of the Swift GRB 210905A", - "textNotes": [ - "\u22c6 Based on observations carried out under ESO prog. ID 106.21T6.010 and ID 106.21T6.015 (PI: N. Tanvir) with the X-shooter spectrograph installed at the Cassegrain focus of the Very Large Telescope (VLT), Unit 3 \u2013 Melipal, operated by the European Southern Observatory (ESO) on Cerro Paranal, Chile. Partly based on observations with the NASA/ESA Hubble Space Telescope, obtained at the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy (AURA). This observation is primarily associated with proposal GO 16918, PI: N. Tanvir." + "editorialHistory": { + "acceptedDate": "2022-11-28", + "receivedDates": [ + "2022-06-07" ] }, - "abstract": { - "textEnglish": "The study of the properties of galaxies in the first billion years after the Big Bang is one of the major topics of current astrophysics. Optical and near-infrared spectroscopy of the afterglows of long gamma-ray bursts (GRBs) provides a powerful diagnostic tool to probe the interstellar medium (ISM) of their host galaxies and foreground absorbers, even up to the highest redshifts. We analyze the VLT/X-shooter afterglow spectrum of GRB 210905A, triggered by the Neil Gehrels Swift Observatory, and detect neutral hydrogen, low-ionization, high-ionization, and fine-structure absorption lines from a complex system at z = 6.3118, which we associate with the GRB host galaxy. We use them to study the ISM properties of the host system, revealing the metallicity, kinematics, and chemical abundance pattern of its gas along the GRB line of sight. We also detect absorption lines from at least two foreground absorbers at z = 5.7390 and z = 2.8296. The total metallicity of the z \u223c 6.3 system is [M/H]tot = \u22121.72 \u00b1 0.13, after correcting for dust depletion and taking \u03b1-element enhancement into account, as suggested by our analysis. This is consistent with the values found for the other two GRBs at z \u223c 6 with spectroscopic data showing metal absorption lines (GRB 050904 and GRB 130606A), and it is at the higher end of the metallicity distribution of quasar damped Lyman-\u03b1 systems (QSO-DLAs) extrapolated to such a high redshift. In addition, we determine the overall amount of dust and dust-to-metal mass ratio (DTM) ([Zn/Fe]fit = 0.33 \u00b1 0.09 and DTM = 0.18 \u00b1 0.03). We find indications of nucleosynthesis due to massive stars and, for some of the components of the gas clouds, we find evidence of peculiar nucleosynthesis, with an overabundance of aluminum (as also found for GRB 130606A). From the analysis of fine-structure lines, we determine distances of several kiloparsecs for the low-ionization gas clouds closest to the GRB. Those are farther distances than usually found for GRB host absorption systems, possibly due to the very high number of ionizing photons produced by the GRB that could ionize the line of sight up to several hundreds of parsecs. Using the HST/F140W image of the GRB field, we show the GRB host galaxy (with a possible afterglow contamination) as well as multiple objects within 2\u2033 from the GRB position. We discuss the galaxy structure and kinematics that could explain our observations, also taking into account a tentative detection of Lyman-\u03b1 emission at z = 6.3449 (\u223c1200 km s\u22121 from the GRB redshift in velocity space), and the observational properties of Lyman-\u03b1 emitters at very high redshift. This study shows the amazing potential of GRBs to access detailed information on the properties (metal enrichment, gas kinematic, dust content, nucleosynthesis...) of very high-redshift galaxies, independently of the galaxy luminosity. Deep spectroscopic observations with VLT/MUSE and JWST will offer the unique possibility of combining the information presented in this paper with the properties of the ionized gas, with the goal of better understanding how galaxies in the reionization era form and evolve." + "esources": [ + { + "location": "https://www.aanda.org/articles/aa/full_html/2023/03/aa44205-22/aa44205-22.html", + "source": "pub_html" + }, + { + "location": "https://www.aanda.org/articles/aa/pdf/2023/03/aa44205-22.pdf", + "source": "pub_pdf" + } + ], + "keywords": [ + { + "keyString": "gamma-ray burst: general", + "keySystem": "misc" + }, + { + "keyString": "gamma-ray burst: individual: GRB 210905A", + "keySystem": "misc" + }, + { + "keyString": "galaxies: abundances", + "keySystem": "misc" + }, + { + "keyString": "galaxies: ISM", + "keySystem": "misc" + }, + { + "keyString": "dust", + "keySystem": "misc" + }, + { + "keyString": "extinction", + "keySystem": "misc" + }, + { + "keyString": "galaxies: high-redshift", + "keySystem": "misc" + } + ], + "openAccess": { + "license": "Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.", + "licenseURL": "https://www.edpsciences.org", + "open": true + }, + "pagination": { + "electronicID": "A84", + "pageCount": "21" + }, + "persistentIDs": [ + { + "DOI": "10.1051/0004-6361/202244205" + } + ], + "pubDate": { + "electrDate": "2023-03-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "0004-6361", + "pubtype": "ppub" + }, + { + "issnString": "1432-0746", + "pubtype": "epub" + } + ], + "issueNum": "None", + "pubName": "Astronomy & Astrophysics", + "pubYear": "2023", + "publisher": "EDP Sciences", + "volumeNum": "671" + }, + "publisherIDs": [ + { + "Identifier": "aa44205-22", + "attribute": "publisher-id" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " Alves-Brito, A., Mel\u00e9ndez, J., Asplund, M., Ram\u00edrez, I., & Yong, D. 2010, A&A, 513, A35 ", @@ -794,53 +834,13 @@ " Zafar, T., & M\u00f8ller, P. 2019, MNRAS, 482, 2731 ", " Zafar, T., P\u00e9roux, C., Popping, A., et al. 2013, A&A, 556, A141 " ], - "esources": [ - { - "source": "pub_html", - "location": "https://www.aanda.org/articles/aa/full_html/2023/03/aa44205-22/aa44205-22.html" - }, - { - "source": "pub_pdf", - "location": "https://www.aanda.org/articles/aa/pdf/2023/03/aa44205-22.pdf" - } - ], - "keywords": [ - { - "keyString": "gamma-ray burst: general", - "keySystem": "misc" - }, - { - "keyString": "gamma-ray burst: individual: GRB 210905A", - "keySystem": "misc" - }, - { - "keyString": "galaxies: abundances", - "keySystem": "misc" - }, - { - "keyString": "galaxies: ISM", - "keySystem": "misc" - }, - { - "keyString": "dust", - "keySystem": "misc" - }, - { - "keyString": "extinction", - "keySystem": "misc" - }, - { - "keyString": "galaxies: high-redshift", - "keySystem": "misc" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 The Authors 2023" + "subtitle": { + "textEnglish": "X-shooter spectroscopy and HST imaging of the afterglow and environment of the Swift GRB 210905A", + "textNotes": [ + "\u22c6 Based on observations carried out under ESO prog. ID 106.21T6.010 and ID 106.21T6.015 (PI: N. Tanvir) with the X-shooter spectrograph installed at the Cassegrain focus of the Very Large Telescope (VLT), Unit 3 \u2013 Melipal, operated by the European Southern Observatory (ESO) on Cerro Paranal, Chile. Partly based on observations with the NASA/ESA Hubble Space Telescope, obtained at the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy (AURA). This observation is primarily associated with proposal GO 16918, PI: N. Tanvir." + ] }, - "openAccess": { - "open": true, - "license": "Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.", - "licenseURL": "https://www.edpsciences.org" + "title": { + "textEnglish": "Dissecting the interstellar medium of a z = 6.3 galaxy" } } diff --git a/tests/stubdata/output/jats_aip_aipc_2470_040010.json b/tests/stubdata/output/jats_aip_aipc_2470_040010.json index 61d1cb8..482e283 100644 --- a/tests/stubdata/output/jats_aip_aipc_2470_040010.json +++ b/tests/stubdata/output/jats_aip_aipc_2470_040010.json @@ -1,62 +1,9 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "printDate": "2022-04-25" - }, - "publication": { - "pubName": "AIP Conference Proceedings", - "confName": "INTERNATIONAL CONFERENCE ON INFORMATICS, TECHNOLOGY, AND ENGINEERING 2021 (InCITE 2021): Leveraging Smart Engineering", - "confLocation": "Surabaya, Indonesia", - "confDates": "25\u201326 August 2021", - "publisher": "AIP Publishing LLC", - "issueNum": "1", - "volumeNum": "2470", - "pubYear": "2022", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "0094-243X" - }, - { - "pubtype": "epub", - "issnString": "1551-7616" - } - ] - }, - "persistentIDs": [ - { - "ISBN": [ - { - "pubtype": "conf-proc", - "isbnString": "978-0-7354-4180-4" - } - ], - "DOI": "10.1063/5.0080203" - } - ], - "publisherIDs": [ - { - "attribute": "manuscript", - "Identifier": "AIPCP21-AR-InCITE2021-00025" - } - ], - "pagination": { - "pageCount": "9", - "electronicID": "040010" + "abstract": { + "textEnglish": "Garlic and chitosan are well-known have an antimicrobial activity to terminate or inhibit the growth of bacteria. This study aims to synthesize, characterize chitosan-garlic film using FTIR, SEM, UV-VIS Spectrophotometry, and swelling analysis; and obtain antimicrobial activity during period time. The variation processes were a type of garlic extract, type of bacteria, and the concentration of garlic extract 1%, 2%, 3%, 10%, and 20%. Chitosan-garlic composite film as a product has an elastic and greasy texture. FTIR analysis shows that chitosan-garlic composite film has ionic interaction between chitosan and garlic extract. The water absorption ability of chitosan-garlic composite film cannot be well determined as not using a crosslinking agent that links garlic extract to composite film. SEM analysis shows the heterogeneous morphology surface of the chitosan-garlic film. Chitosan-garlic powder composite film at 20% concentration (b/v) tested against S. aureus has the highest antimicrobial activity with OD600 0,001342. Chitosan-garlic oil composite film at 20% concentration (v/v) tested against S. aureus has the highest antimicrobial activity with OD600 0,0013. Spectrophotometry UV-VIS method confirmed that the antimicrobial activity of chitosan-garlic composite film increased compared to the concentration of garlic extract and decreased compared to storage time. The elasticity of chitosan-garlic composite film decreased compared to the concentration of garlic extract." }, "authors": [ { - "name": { - "surname": "Savitri", - "given_name": "Emma" - }, "affiliation": [ { "affPubRaw": "Chemical Engineering Department, University of Surabaya, Surabaya 60293, Indonesia" @@ -64,94 +11,157 @@ ], "attrib": { "email": "savitri_ma@staff.ubaya.ac.id" + }, + "name": { + "given_name": "Emma", + "surname": "Savitri" } }, { - "name": { - "surname": "Tjahayani", - "given_name": "Maria Irine" - }, "affiliation": [ { "affPubRaw": "Chemical Engineering Department, University of Surabaya, Surabaya 60293, Indonesia" } - ] + ], + "name": { + "given_name": "Maria Irine", + "surname": "Tjahayani" + } }, { - "name": { - "surname": "Say", - "given_name": "Anastasia Apriyani Ngene" - }, "affiliation": [ { "affPubRaw": "Chemical Engineering Department, University of Surabaya, Surabaya 60293, Indonesia" } - ] + ], + "name": { + "given_name": "Anastasia Apriyani Ngene", + "surname": "Say" + } } ], + "copyright": { + "statement": "\u00a9 2022 Author(s)", + "status": true + }, + "keywords": [ + { + "keyString": "POWER SYSTEM AND SMART ENERGY MANAGEMENT", + "keySystem": "subject" + } + ], + "openAccess": { + "license": "Published by AIP Publishing." + }, "otherContributor": [ { - "role": "Conference Editor", "contrib": { - "name": { - "surname": "Parung", - "given_name": "Joniarto" - }, "affiliation": [ { "affPubRaw": "Universitas Surabaya, Surabaya, Indonesia" } - ] - } + ], + "name": { + "given_name": "Joniarto", + "surname": "Parung" + } + }, + "role": "Conference Editor" }, { - "role": "Conference Editor", "contrib": { - "name": { - "surname": "Pah", - "given_name": "Nemuel Daniel" - }, "affiliation": [ { "affPubRaw": "Universitas Surabaya, Surabaya, Indonesia" } - ] - } + ], + "name": { + "given_name": "Nemuel Daniel", + "surname": "Pah" + } + }, + "role": "Conference Editor" }, { - "role": "Conference Editor", "contrib": { - "name": { - "surname": "Sutrisna", - "given_name": "Putu Doddy" - }, "affiliation": [ { "affPubRaw": "Universitas Surabaya, Surabaya, Indonesia" } - ] - } + ], + "name": { + "given_name": "Putu Doddy", + "surname": "Sutrisna" + } + }, + "role": "Conference Editor" }, { - "role": "Conference Editor", "contrib": { - "name": { - "surname": "Suciadi", - "given_name": "Marcellinus Ferdinand" - }, "affiliation": [ { "affPubRaw": "Universitas Surabaya, Surabaya, Indonesia" } - ] - } + ], + "name": { + "given_name": "Marcellinus Ferdinand", + "surname": "Suciadi" + } + }, + "role": "Conference Editor" } ], - "title": { - "textEnglish": "Synthesis and characterization of chitosan-Allium sativum film" + "pagination": { + "electronicID": "040010", + "pageCount": "9" }, - "abstract": { - "textEnglish": "Garlic and chitosan are well-known have an antimicrobial activity to terminate or inhibit the growth of bacteria. This study aims to synthesize, characterize chitosan-garlic film using FTIR, SEM, UV-VIS Spectrophotometry, and swelling analysis; and obtain antimicrobial activity during period time. The variation processes were a type of garlic extract, type of bacteria, and the concentration of garlic extract 1%, 2%, 3%, 10%, and 20%. Chitosan-garlic composite film as a product has an elastic and greasy texture. FTIR analysis shows that chitosan-garlic composite film has ionic interaction between chitosan and garlic extract. The water absorption ability of chitosan-garlic composite film cannot be well determined as not using a crosslinking agent that links garlic extract to composite film. SEM analysis shows the heterogeneous morphology surface of the chitosan-garlic film. Chitosan-garlic powder composite film at 20% concentration (b/v) tested against S. aureus has the highest antimicrobial activity with OD600 0,001342. Chitosan-garlic oil composite film at 20% concentration (v/v) tested against S. aureus has the highest antimicrobial activity with OD600 0,0013. Spectrophotometry UV-VIS method confirmed that the antimicrobial activity of chitosan-garlic composite film increased compared to the concentration of garlic extract and decreased compared to storage time. The elasticity of chitosan-garlic composite film decreased compared to the concentration of garlic extract." + "persistentIDs": [ + { + "DOI": "10.1063/5.0080203", + "ISBN": [ + { + "isbnString": "978-0-7354-4180-4", + "pubtype": "conf-proc" + } + ] + } + ], + "pubDate": { + "printDate": "2022-04-25" + }, + "publication": { + "ISSN": [ + { + "issnString": "0094-243X", + "pubtype": "ppub" + }, + { + "issnString": "1551-7616", + "pubtype": "epub" + } + ], + "confDates": "25\u201326 August 2021", + "confLocation": "Surabaya, Indonesia", + "confName": "INTERNATIONAL CONFERENCE ON INFORMATICS, TECHNOLOGY, AND ENGINEERING 2021 (InCITE 2021): Leveraging Smart Engineering", + "issueNum": "1", + "pubName": "AIP Conference Proceedings", + "pubYear": "2022", + "publisher": "AIP Publishing LLC", + "volumeNum": "2470" + }, + "publisherIDs": [ + { + "Identifier": "AIPCP21-AR-InCITE2021-00025", + "attribute": "manuscript" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ "S. Qomariah, Lisdiana, and W. Christijanti, Unnes Journal of Life Science, 79, (2014).", @@ -172,17 +182,7 @@ "A. Lucas, A. Pengaruh Plasticizer terhadap Sifat Mekanik dan Struktur Kimia Film Kitosan-Pati. Penelitian. (2010)", "A.M. Far\u00edas-Campomanes, C. N. Horita, M.A.R. Pollonio, M. A. A. Meireles. Allicin-Rich Extract Obtained from Garlic by Pressurized Liquid Extraction: Quantitative Determination of Allicin in Garlic Samples, Food and Public Health 4(6): 272\u2013278 (2014)" ], - "keywords": [ - { - "keyString": "POWER SYSTEM AND SMART ENERGY MANAGEMENT", - "keySystem": "subject" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 2022 Author(s)" - }, - "openAccess": { - "license": "Published by AIP Publishing." + "title": { + "textEnglish": "Synthesis and characterization of chitosan-Allium sativum film" } } diff --git a/tests/stubdata/output/jats_aip_amjph_90_286.json b/tests/stubdata/output/jats_aip_amjph_90_286.json index 0919972..35bc14e 100644 --- a/tests/stubdata/output/jats_aip_amjph_90_286.json +++ b/tests/stubdata/output/jats_aip_amjph_90_286.json @@ -1,61 +1,9 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2020-11-19" - ], - "acceptedDate": "2021-12-07" - }, - "pubDate": { - "printDate": "2022-04-00" - }, - "publication": { - "pubName": "American Journal of Physics", - "publisher": "American Association of Physics Teachers", - "issueNum": "4", - "volumeNum": "90", - "pubYear": "2022", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "0002-9505" - }, - { - "pubtype": "epub", - "issnString": "1943-2909" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1119/10.0009409" - } - ], - "publisherIDs": [ - { - "attribute": "manuscript", - "Identifier": "AJP22-AR-00002" - } - ], - "pagination": { - "firstPage": "286", - "lastPage": "296", - "pageCount": "11", - "pageRange": "286-296" + "abstract": { + "textEnglish": "Gravitational-wave observatories around the world are searching for continuous waves: persistent signals from sources, such as spinning neutron stars. These searches use sophisticated statistical techniques to look for weak signals in noisy data. In this paper, we demonstrate these techniques using a table-top model gravitational-wave detector: a Michelson interferometer where sound is used as an analog for gravitational waves. Using signal processing techniques from continuous-wave searches, we demonstrate the recovery of tones with constant and wandering frequencies. We also explore the use of the interferometer as a teaching tool for educators in physics and electrical engineering by using it as an \u201coptical microphone\u201d to capture music and speech. A range of filtering techniques used to recover signals from noisy data are detailed in the supplementary material of this article. Here, we present the highlights of our results using a combined notch plus Wiener filter and the statistical log minimum mean-square error (logMMSE) estimator. Using these techniques, we easily recover recordings of simple chords and drums, but complex music and speech are more challenging. This demonstration can be used by educators in undergraduate laboratories and can be adapted for communicating gravitational-wave and signal-processing topics to nonspecialist audiences." }, "authors": [ { - "name": { - "surname": "Gardner", - "given_name": "James W." - }, "affiliation": [ { "affPubRaw": "Centre for Gravitational Astrophysics, The Australian National University , Acton, ACT 2601, Australia ;" @@ -63,79 +11,79 @@ { "affPubRaw": "OzGrav-ANU, Australian Research Council Centre of Excellence for Gravitational Wave Discovery, The Australian National University , Acton, ACT 2601, Australia ; and School of Physics, University of Melbourne , Parkville, Victoria 3010, Australia" } - ] + ], + "name": { + "given_name": "James W.", + "surname": "Gardner" + } }, { - "name": { - "surname": "Middleton", - "given_name": "Hannah" - }, "affiliation": [ { "affPubRaw": "School of Physics, University of Melbourne, Parkville, Victoria 3010, Australia; Centre for Astrophysics and Supercomputing, Swinburne University of Technology , Hawthorn, Victoria 3122, Australia ; OzGrav-Melbourne, Australian Research Council Centre of Excellence for Gravitational Wave Discovery , Parkville, Victoria 3010, Australia ; and School of Physics and Astronomy and Institute for Gravitational Wave Astronomy, University of Birmingham, Edgbaston, Birmingham, B15 9TT, United Kingdom" } - ] + ], + "name": { + "given_name": "Hannah", + "surname": "Middleton" + } }, { - "name": { - "surname": "Liu", - "given_name": "Changrong" - }, "affiliation": [ { "affPubRaw": "Department of Electrical and Electronic Engineering, University of Melbourne, Parkville, Victoria 3010, Australia and OzGrav-Melbourne, Australian Research Council Centre of Excellence for Gravitational Wave Discovery , Parkville, Victoria 3010, Australia" } - ] + ], + "name": { + "given_name": "Changrong", + "surname": "Liu" + } }, { - "name": { - "surname": "Melatos", - "given_name": "Andrew" - }, "affiliation": [ { "affPubRaw": "School of Physics, University of Melbourne , Parkville, Victoria 3010, Australia and OzGrav-Melbourne, Australian Research Council Centre of Excellence for Gravitational Wave Discovery , Parkville, Victoria 3010, Australia" } - ] + ], + "name": { + "given_name": "Andrew", + "surname": "Melatos" + } }, { - "name": { - "surname": "Evans", - "given_name": "Robin" - }, "affiliation": [ { "affPubRaw": "Department of Electrical and Electronic Engineering, University of Melbourne, Parkville, Victoria 3010, Australia and OzGrav-Melbourne, Australian Research Council Centre of Excellence for Gravitational Wave Discovery , Parkville, Victoria 3010, Australia" } - ] + ], + "name": { + "given_name": "Robin", + "surname": "Evans" + } }, { - "name": { - "surname": "Moran", - "given_name": "William" - }, "affiliation": [ { "affPubRaw": "Department of Electrical and Electronic Engineering, University of Melbourne , Parkville, Victoria 3010, Australia" } - ] + ], + "name": { + "given_name": "William", + "surname": "Moran" + } }, { - "name": { - "surname": "Beniwal", - "given_name": "Deeksha" - }, "affiliation": [ { "affPubRaw": "Department of Physics, The University of Adelaide , Adelaide, South Australia 5005, Australia ; The Institute of Photonics and Advanced Sensing (IPAS), The University of Adelaide , Adelaide, South Australia 5005, Australia ; and OzGrav-Adelaide, Australian Research Council Centre of Excellence for Gravitational Wave Discovery , Adelaide, South Australia 5005, Australia" } - ] + ], + "name": { + "given_name": "Deeksha", + "surname": "Beniwal" + } }, { - "name": { - "surname": "Cao", - "given_name": "Huy Tuong" - }, "affiliation": [ { "affPubRaw": "Department of Physics, The University of Adelaide , Adelaide, South Australia 5005, Australia ;" @@ -143,47 +91,109 @@ { "affPubRaw": "The Institute of Photonics and Advanced Sensing (IPAS), The University of Adelaide , Adelaide, South Australia 5005, Australia ; and OzGrav-Adelaide, Australian Research Council Centre of Excellence for Gravitational Wave Discovery , Adelaide, South Australia 5005, Australia" } - ] + ], + "name": { + "given_name": "Huy Tuong", + "surname": "Cao" + } }, { - "name": { - "surname": "Ingram", - "given_name": "Craig" - }, "affiliation": [ { "affPubRaw": "Department of Physics, The University of Adelaide , Adelaide, South Australia 5005, Australia ; The Institute of Photonics and Advanced Sensing (IPAS), The University of Adelaide , Adelaide, South Australia 5005, Australia ; and OzGrav-Adelaide, Australian Research Council Centre of Excellence for Gravitational Wave Discovery , Adelaide, South Australia 5005, Australia" } - ] + ], + "name": { + "given_name": "Craig", + "surname": "Ingram" + } }, { - "name": { - "surname": "Brown", - "given_name": "Daniel" - }, "affiliation": [ { "affPubRaw": "Department of Physics, The University of Adelaide , Adelaide, South Australia 5005, Australia ; The Institute of Photonics and Advanced Sensing (IPAS), The University of Adelaide , Adelaide, South Australia 5005, Australia ; and OzGrav-Adelaide, Australian Research Council Centre of Excellence for Gravitational Wave Discovery , Adelaide, South Australia 5005, Australia" } - ] + ], + "name": { + "given_name": "Daniel", + "surname": "Brown" + } }, { - "name": { - "surname": "Ng", - "given_name": "Sebastian" - }, "affiliation": [ { "affPubRaw": "Department of Physics, The University of Adelaide , Adelaide, South Australia 5005, Australia ; The Institute of Photonics and Advanced Sensing (IPAS), The University of Adelaide , Adelaide, South Australia 5005, Australia ; and OzGrav-Adelaide, Australian Research Council Centre of Excellence for Gravitational Wave Discovery , Adelaide, South Australia 5005, Australia" } - ] + ], + "name": { + "given_name": "Sebastian", + "surname": "Ng" + } } ], - "title": { - "textEnglish": "Continuous gravitational waves in the lab: Recovering audio signals with a table-top optical microphone" + "copyright": { + "statement": "\u00a9 2022 Author(s).", + "status": true }, - "abstract": { - "textEnglish": "Gravitational-wave observatories around the world are searching for continuous waves: persistent signals from sources, such as spinning neutron stars. These searches use sophisticated statistical techniques to look for weak signals in noisy data. In this paper, we demonstrate these techniques using a table-top model gravitational-wave detector: a Michelson interferometer where sound is used as an analog for gravitational waves. Using signal processing techniques from continuous-wave searches, we demonstrate the recovery of tones with constant and wandering frequencies. We also explore the use of the interferometer as a teaching tool for educators in physics and electrical engineering by using it as an \u201coptical microphone\u201d to capture music and speech. A range of filtering techniques used to recover signals from noisy data are detailed in the supplementary material of this article. Here, we present the highlights of our results using a combined notch plus Wiener filter and the statistical log minimum mean-square error (logMMSE) estimator. Using these techniques, we easily recover recordings of simple chords and drums, but complex music and speech are more challenging. This demonstration can be used by educators in undergraduate laboratories and can be adapted for communicating gravitational-wave and signal-processing topics to nonspecialist audiences." + "editorialHistory": { + "acceptedDate": "2021-12-07", + "receivedDates": [ + "2020-11-19" + ] + }, + "keywords": [ + { + "keyString": "PAPERS", + "keySystem": "subject" + } + ], + "openAccess": { + "license": "Published under an exclusive license by American Association of Physics Teachers." + }, + "pagination": { + "firstPage": "286", + "lastPage": "296", + "pageCount": "11", + "pageRange": "286-296" + }, + "persistentIDs": [ + { + "DOI": "10.1119/10.0009409" + } + ], + "pubDate": { + "printDate": "2022-04-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "0002-9505", + "pubtype": "ppub" + }, + { + "issnString": "1943-2909", + "pubtype": "epub" + } + ], + "issueNum": "4", + "pubName": "American Journal of Physics", + "pubYear": "2022", + "publisher": "American Association of Physics Teachers", + "volumeNum": "90" + }, + "publisherIDs": [ + { + "Identifier": "AJP22-AR-00002", + "attribute": "manuscript" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " B. P. Abbott , R. Abbott , T. D. Abbott et al., \u201c Observation of gravitational waves from a binary black hole merger,\u201d Phys. Rev. Lett. 116, 061102 (2016).10.1103/PhysRevLett.116.061102 ", @@ -213,17 +223,7 @@ " E. T. Jaynes , Probability Theory: The Logic of Science ( Cambridge U. P., Cambridge, 2003). ", " See supplementary material at https://www.scitation.org/doi/suppl/10.1119/10.0009409 for further resources and a detailed explanation and discussion of the different signal-processing techniques used for speech enhancement of the recordings from the optical microphone, including techniques not presented in the main text. " ], - "keywords": [ - { - "keyString": "PAPERS", - "keySystem": "subject" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 2022 Author(s)." - }, - "openAccess": { - "license": "Published under an exclusive license by American Association of Physics Teachers." + "title": { + "textEnglish": "Continuous gravitational waves in the lab: Recovering audio signals with a table-top optical microphone" } } diff --git a/tests/stubdata/output/jats_aj_158_4_139.json b/tests/stubdata/output/jats_aj_158_4_139.json index 50314e8..a35d6f0 100644 --- a/tests/stubdata/output/jats_aj_158_4_139.json +++ b/tests/stubdata/output/jats_aj_158_4_139.json @@ -1,334 +1,367 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2019-04-06" - ], - "revisedDates": [ - "2019-07-23" - ], - "acceptedDate": "2019-07-25" - }, - "pubDate": { - "electrDate": "2019-09-09", - "printDate": "2019-10-00" - }, - "publication": { - "pubName": "The Astronomical Journal", - "publisher": "The American Astronomical Society", - "issueNum": "4", - "volumeNum": "158", - "pubYear": "2019", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "0004-6256" - }, - { - "pubtype": "epub", - "issnString": "1538-3881" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.3847/1538-3881/ab3643" - } - ], - "publisherIDs": [ - { - "attribute": "publisher-id", - "Identifier": "ajab3643" - }, - { - "attribute": "manuscript", - "Identifier": "ab3643" - }, - { - "attribute": "other", - "Identifier": "AAS17124" - } - ], - "pagination": { - "pageCount": "17", - "electronicID": "139" + "abstract": { + "textEnglish": "We obtained the first maps of Jupiter at 13 mm wavelength with the Atacama Large Millimeter/Submillimeter Array (ALMA) on 2017 January 35, just days after an energetic eruption at 165S jovigraphic latitude had been reported by the amateur community, and about two to three months after the detection of similarly energetic eruptions in the northern hemisphere, at 222230N. Our observations, probing below the ammonia cloud deck, show that the erupting plumes in the South Equatorial Belt bring up ammonia gas from the deep atmosphere. While models of plume eruptions that are triggered at the water condensation level explain data taken at uvvisible and mid-infrared wavelengths, our ALMA observations provide a crucial, hitherto missing, link in the moist convection theory by showing that ammonia gas from the deep atmosphere is indeed brought up in these plumes. Contemporaneous Hubble Space Telescope data show that the plumes reach altitudes as high as the tropopause. We suggest that the plumes at 222230N also rise up well above the ammonia cloud deck and that descending air may dry the neighboring belts even more than in quiescent times, which would explain our observations in the north." }, "authors": [ { - "name": { - "surname": "de Pater", - "given_name": "Imke" - }, "affiliation": [ { - "affPubRaw": "Department of Astronomy, 501 Campbell Hall, University of California, Berkeley, CA 94720, USA", - "affPubID": "ajab3643af1" + "affPubID": "ajab3643af1", + "affPubRaw": "Department of Astronomy, 501 Campbell Hall, University of California, Berkeley, CA 94720, USA" } ], "attrib": { "email": "imke@berkeley.edu", "orcid": "0000-0002-4278-3168" + }, + "name": { + "given_name": "Imke", + "surname": "de Pater" } }, { - "name": { - "surname": "Sault", - "given_name": "R. J." - }, "affiliation": [ { - "affPubRaw": "School of Physics, University of Melbourne, Victoria, 3010, Australia", - "affPubID": "ajab3643af2" + "affPubID": "ajab3643af2", + "affPubRaw": "School of Physics, University of Melbourne, Victoria, 3010, Australia" } ], "attrib": { "orcid": "0000-0001-9209-7716" + }, + "name": { + "given_name": "R. J.", + "surname": "Sault" } }, { - "name": { - "surname": "Moeckel", - "given_name": "Chris" - }, "affiliation": [ { - "affPubRaw": "Department of Earth and Planetary Sciences, McCone Hall, University of California, Berkeley, CA 94720, USA", - "affPubID": "ajab3643af3" + "affPubID": "ajab3643af3", + "affPubRaw": "Department of Earth and Planetary Sciences, McCone Hall, University of California, Berkeley, CA 94720, USA" } - ] + ], + "name": { + "given_name": "Chris", + "surname": "Moeckel" + } }, { - "name": { - "surname": "Moullet", - "given_name": "Arielle" - }, "affiliation": [ { - "affPubRaw": "SOFIA/USRA, NASA Ames Building N232, Moffett Field, CA 94035, USA", - "affPubID": "ajab3643af4" + "affPubID": "ajab3643af4", + "affPubRaw": "SOFIA/USRA, NASA Ames Building N232, Moffett Field, CA 94035, USA" } - ] + ], + "name": { + "given_name": "Arielle", + "surname": "Moullet" + } }, { - "name": { - "surname": "Wong", - "given_name": "Michael H." - }, "affiliation": [ { - "affPubRaw": "Department of Astronomy, 501 Campbell Hall, University of California, Berkeley, CA 94720, USA", - "affPubID": "ajab3643af1" + "affPubID": "ajab3643af1", + "affPubRaw": "Department of Astronomy, 501 Campbell Hall, University of California, Berkeley, CA 94720, USA" } ], "attrib": { "orcid": "0000-0003-2804-5086" + }, + "name": { + "given_name": "Michael H.", + "surname": "Wong" } }, { - "name": { - "surname": "Goullaud", - "given_name": "Charles" - }, "affiliation": [ { - "affPubRaw": "Department of Astronomy, 501 Campbell Hall, University of California, Berkeley, CA 94720, USA", - "affPubID": "ajab3643af1" + "affPubID": "ajab3643af1", + "affPubRaw": "Department of Astronomy, 501 Campbell Hall, University of California, Berkeley, CA 94720, USA" } - ] + ], + "name": { + "given_name": "Charles", + "surname": "Goullaud" + } }, { - "name": { - "surname": "DeBoer", - "given_name": "David" - }, "affiliation": [ { - "affPubRaw": "Department of Astronomy, 501 Campbell Hall, University of California, Berkeley, CA 94720, USA", - "affPubID": "ajab3643af1" + "affPubID": "ajab3643af1", + "affPubRaw": "Department of Astronomy, 501 Campbell Hall, University of California, Berkeley, CA 94720, USA" } ], "attrib": { "orcid": "0000-0003-3197-2294" + }, + "name": { + "given_name": "David", + "surname": "DeBoer" } }, { - "name": { - "surname": "Butler", - "given_name": "Bryan J." - }, "affiliation": [ { - "affPubRaw": "National Radio Astronomy Observatory, Socorro, NM 87801, USA", - "affPubID": "ajab3643af5" + "affPubID": "ajab3643af5", + "affPubRaw": "National Radio Astronomy Observatory, Socorro, NM 87801, USA" } ], "attrib": { "orcid": "0000-0002-5344-820X" + }, + "name": { + "given_name": "Bryan J.", + "surname": "Butler" } }, { - "name": { - "surname": "Bjoraker", - "given_name": "Gordon" - }, "affiliation": [ { - "affPubRaw": "Goddard Space Flight Center, 8800 Greenbelt Road, Greenbelt MD 20771, USA", - "affPubID": "ajab3643af6" + "affPubID": "ajab3643af6", + "affPubRaw": "Goddard Space Flight Center, 8800 Greenbelt Road, Greenbelt MD 20771, USA" } ], "attrib": { "orcid": "0000-0002-9679-4153" + }, + "name": { + "given_name": "Gordon", + "surname": "Bjoraker" } }, { - "name": { - "surname": "dmkovics", - "given_name": "Mt" - }, "affiliation": [ { - "affPubRaw": "Dept. of Physics & Astronomy, Clemson University, Clemson, SC 29634-0978, USA", - "affPubID": "ajab3643af7" + "affPubID": "ajab3643af7", + "affPubRaw": "Dept. of Physics & Astronomy, Clemson University, Clemson, SC 29634-0978, USA" } ], "attrib": { "orcid": "0000-0003-1869-0938" + }, + "name": { + "given_name": "Mt", + "surname": "dmkovics" } }, { - "name": { - "surname": "Cosentino", - "given_name": "Richard" - }, "affiliation": [ { - "affPubRaw": "Goddard Space Flight Center, 8800 Greenbelt Road, Greenbelt MD 20771, USA", - "affPubID": "ajab3643af6" + "affPubID": "ajab3643af6", + "affPubRaw": "Goddard Space Flight Center, 8800 Greenbelt Road, Greenbelt MD 20771, USA" } ], "attrib": { "orcid": "0000-0003-3047-615X" + }, + "name": { + "given_name": "Richard", + "surname": "Cosentino" } }, { - "name": { - "surname": "Donnelly", - "given_name": "Padraig T." - }, "affiliation": [ { - "affPubRaw": "Department of Physics and Astronomy, University of Leicester, University Road, Leicester, LE1 7RH, UK", - "affPubID": "ajab3643af8" + "affPubID": "ajab3643af8", + "affPubRaw": "Department of Physics and Astronomy, University of Leicester, University Road, Leicester, LE1 7RH, UK" } ], "attrib": { "orcid": "0000-0002-4241-0302" + }, + "name": { + "given_name": "Padraig T.", + "surname": "Donnelly" } }, { - "name": { - "surname": "Fletcher", - "given_name": "Leigh N." - }, "affiliation": [ { - "affPubRaw": "Department of Physics and Astronomy, University of Leicester, University Road, Leicester, LE1 7RH, UK", - "affPubID": "ajab3643af8" + "affPubID": "ajab3643af8", + "affPubRaw": "Department of Physics and Astronomy, University of Leicester, University Road, Leicester, LE1 7RH, UK" } ], "attrib": { "orcid": "0000-0001-5834-9588" + }, + "name": { + "given_name": "Leigh N.", + "surname": "Fletcher" } }, { - "name": { - "surname": "Kasaba", - "given_name": "Yasumasa" - }, "affiliation": [ { - "affPubRaw": "Planetary Plasma and Atmospheric Research Center (PPARC), Tohoku University, Japan", - "affPubID": "ajab3643af9" + "affPubID": "ajab3643af9", + "affPubRaw": "Planetary Plasma and Atmospheric Research Center (PPARC), Tohoku University, Japan" } ], "attrib": { "orcid": "0000-0002-8160-3553" + }, + "name": { + "given_name": "Yasumasa", + "surname": "Kasaba" } }, { - "name": { - "surname": "Orton", - "given_name": "Glenn S." - }, "affiliation": [ { - "affPubRaw": "Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena, CA 91109, USA", - "affPubID": "ajab3643af10" + "affPubID": "ajab3643af10", + "affPubRaw": "Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena, CA 91109, USA" } ], "attrib": { "orcid": "0000-0001-7871-2823" + }, + "name": { + "given_name": "Glenn S.", + "surname": "Orton" } }, { - "name": { - "surname": "Rogers", - "given_name": "John H." - }, "affiliation": [ { - "affPubRaw": "British Astronomical Association, Burlington House, Piccadilly, London W1J 0DU, UK", - "affPubID": "ajab3643af11" + "affPubID": "ajab3643af11", + "affPubRaw": "British Astronomical Association, Burlington House, Piccadilly, London W1J 0DU, UK" } ], "attrib": { "orcid": "0000-0002-4239-5907" + }, + "name": { + "given_name": "John H.", + "surname": "Rogers" } }, { - "name": { - "surname": "Sinclair", - "given_name": "James A." - }, "affiliation": [ { - "affPubRaw": "Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena, CA 91109, USA", - "affPubID": "ajab3643af10" + "affPubID": "ajab3643af10", + "affPubRaw": "Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena, CA 91109, USA" } ], "attrib": { "orcid": "0000-0001-5374-4028" + }, + "name": { + "given_name": "James A.", + "surname": "Sinclair" } }, { - "name": { - "surname": "Villard", - "given_name": "Eric" - }, "affiliation": [ { - "affPubRaw": "Joint ALMA Observatory/ESO, Avenida Alonso de Cordova 3107, Vitacura, Santiago, Chile", - "affPubID": "ajab3643af12" + "affPubID": "ajab3643af12", + "affPubRaw": "Joint ALMA Observatory/ESO, Avenida Alonso de Cordova 3107, Vitacura, Santiago, Chile" } ], "attrib": { "orcid": "0000-0003-4314-4947" + }, + "name": { + "given_name": "Eric", + "surname": "Villard" } } ], - "title": { - "textEnglish": "First ALMA Millimeter-wavelength Maps of Jupiter, with a Multiwavelength Study of Convection" + "copyright": { + "statement": "2019. The American Astronomical Society. All rights reserved.", + "status": true }, - "abstract": { - "textEnglish": "We obtained the first maps of Jupiter at 13 mm wavelength with the Atacama Large Millimeter/Submillimeter Array (ALMA) on 2017 January 35, just days after an energetic eruption at 165S jovigraphic latitude had been reported by the amateur community, and about two to three months after the detection of similarly energetic eruptions in the northern hemisphere, at 222230N. Our observations, probing below the ammonia cloud deck, show that the erupting plumes in the South Equatorial Belt bring up ammonia gas from the deep atmosphere. While models of plume eruptions that are triggered at the water condensation level explain data taken at uvvisible and mid-infrared wavelengths, our ALMA observations provide a crucial, hitherto missing, link in the moist convection theory by showing that ammonia gas from the deep atmosphere is indeed brought up in these plumes. Contemporaneous Hubble Space Telescope data show that the plumes reach altitudes as high as the tropopause. We suggest that the plumes at 222230N also rise up well above the ammonia cloud deck and that descending air may dry the neighboring belts even more than in quiescent times, which would explain our observations in the north." + "editorialHistory": { + "acceptedDate": "2019-07-25", + "receivedDates": [ + "2019-04-06" + ], + "revisedDates": [ + "2019-07-23" + ] + }, + "funding": [ + { + "agencyname": "NASA", + "awardnumber": "80NSSC18K1001" + }, + { + "agencyname": "NRAO", + "awardnumber": "NRAO Student Observing Support (SOS) Program" + } + ], + "keywords": [ + { + "keyString": "methods: observational", + "keySystem": "AAS" + }, + { + "keyString": "planets and satellites: atmospheres", + "keySystem": "AAS" + }, + { + "keyString": "radiative transfer", + "keySystem": "AAS" + }, + { + "keyString": "radio continuum: planetary systems", + "keySystem": "AAS" + }, + { + "keyString": "techniques: interferometric", + "keySystem": "AAS" + } + ], + "pagination": { + "electronicID": "139", + "pageCount": "17" + }, + "persistentIDs": [ + { + "DOI": "10.3847/1538-3881/ab3643" + } + ], + "pubDate": { + "electrDate": "2019-09-09", + "printDate": "2019-10-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "0004-6256", + "pubtype": "ppub" + }, + { + "issnString": "1538-3881", + "pubtype": "epub" + } + ], + "issueNum": "4", + "pubName": "The Astronomical Journal", + "pubYear": "2019", + "publisher": "The American Astronomical Society", + "volumeNum": "158" + }, + "publisherIDs": [ + { + "Identifier": "ajab3643", + "attribute": "publisher-id" + }, + { + "Identifier": "ab3643", + "attribute": "manuscript" + }, + { + "Identifier": "AAS17124", + "attribute": "other" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " dmkovics M. Mitchell J. L. Hayes A. G. 2016 Icar 270 376 2016Icar..270..376A 10.1016/j.icarus.2015.05.023 ", @@ -388,40 +421,7 @@ " Wong M. H. Atreya S. K. Kuhn W. R. Romani P. N. Mihalka K. M. 2015 Icar 245 273 2015Icar..245..273W 10.1016/j.icarus.2014.09.042 ", " Wong M. H. Mahaffy P. R. Atreya S. K. Niemann H. B. Owen T. C. 2004 Icar 171 153 2004Icar..171..153W 10.1016/j.icarus.2004.04.010 " ], - "keywords": [ - { - "keyString": "methods: observational", - "keySystem": "AAS" - }, - { - "keyString": "planets and satellites: atmospheres", - "keySystem": "AAS" - }, - { - "keyString": "radiative transfer", - "keySystem": "AAS" - }, - { - "keyString": "radio continuum: planetary systems", - "keySystem": "AAS" - }, - { - "keyString": "techniques: interferometric", - "keySystem": "AAS" - } - ], - "copyright": { - "status": true, - "statement": "2019. The American Astronomical Society. All rights reserved." - }, - "funding": [ - { - "agencyname": "NASA", - "awardnumber": "80NSSC18K1001" - }, - { - "agencyname": "NRAO", - "awardnumber": "NRAO Student Observing Support (SOS) Program" - } - ] + "title": { + "textEnglish": "First ALMA Millimeter-wavelength Maps of Jupiter, with a Multiwavelength Study of Convection" + } } diff --git a/tests/stubdata/output/jats_aj_158_4_139_fulltext.json b/tests/stubdata/output/jats_aj_158_4_139_fulltext.json index 6310659..0d1af18 100644 --- a/tests/stubdata/output/jats_aj_158_4_139_fulltext.json +++ b/tests/stubdata/output/jats_aj_158_4_139_fulltext.json @@ -1,8 +1,14 @@ -{"unresolved":{ - "ajab3643bib21": ["Fortuitously, the timing of the ALMA observations [...] The last full fade and revival cycle of the SEB took place in 20092011 (Fletcher et al. 2011, 2017a), where the word fading is used when the SEB loses its brown color and turns white [...]"], - "ajab3643bib22": [ - "Fortuitously, the timing of the ALMA observations [...] The last full fade and revival cycle of the SEB took place in 20092011 (Fletcher et al. 2011, 2017a), where the word fading is used when the SEB loses its brown color and turns white [...]", - "ALMA observed Jupiter just a few days after an outbreak [...] The event shows a strong resemblance with the SEB revival in 20102011 (Fletcher et al. 2017a), a series of convective events [...]At mid-IR wavelengths [...] Such a stratospheric thermal wave was clearly present during the 20102011 SEB revival (Fletcher et al. 2017a).", - "ALMA observed Jupiter just a few days after an outbreak [...] The event shows a strong resemblance with the SEB revival in 20102011 (Fletcher et al. 2017a), a series of convective events [...]At mid-IR wavelengths [...] Such a stratospheric thermal wave was clearly present during the 20102011 SEB revival (Fletcher et al. 2017a).Fletcher et al. (2017a) compared the convective eruptions triggering the 20102011 SEB revival with mesoscale convective storms (MCS) seen on Earth [...]", - "At mid-IR wavelengths [...] Such a stratospheric thermal wave was clearly present during the 20102011 SEB revival (Fletcher et al. 2017a).Fletcher et al. (2017a) compared the convective eruptions triggering the 20102011 SEB revival with mesoscale convective storms (MCS) seen on Earth [...]"]}, -"resolved": {}} +{ + "resolved": {}, + "unresolved": { + "ajab3643bib21": [ + "Fortuitously, the timing of the ALMA observations [...] The last full fade and revival cycle of the SEB took place in 20092011 (Fletcher et al. 2011, 2017a), where the word fading is used when the SEB loses its brown color and turns white [...]" + ], + "ajab3643bib22": [ + "Fortuitously, the timing of the ALMA observations [...] The last full fade and revival cycle of the SEB took place in 20092011 (Fletcher et al. 2011, 2017a), where the word fading is used when the SEB loses its brown color and turns white [...]", + "ALMA observed Jupiter just a few days after an outbreak [...] The event shows a strong resemblance with the SEB revival in 20102011 (Fletcher et al. 2017a), a series of convective events [...]At mid-IR wavelengths [...] Such a stratospheric thermal wave was clearly present during the 20102011 SEB revival (Fletcher et al. 2017a).", + "ALMA observed Jupiter just a few days after an outbreak [...] The event shows a strong resemblance with the SEB revival in 20102011 (Fletcher et al. 2017a), a series of convective events [...]At mid-IR wavelengths [...] Such a stratospheric thermal wave was clearly present during the 20102011 SEB revival (Fletcher et al. 2017a).Fletcher et al. (2017a) compared the convective eruptions triggering the 20102011 SEB revival with mesoscale convective storms (MCS) seen on Earth [...]", + "At mid-IR wavelengths [...] Such a stratospheric thermal wave was clearly present during the 20102011 SEB revival (Fletcher et al. 2017a).Fletcher et al. (2017a) compared the convective eruptions triggering the 20102011 SEB revival with mesoscale convective storms (MCS) seen on Earth [...]" + ] + } +} diff --git a/tests/stubdata/output/jats_aj_158_4_139_fulltext_tags.json b/tests/stubdata/output/jats_aj_158_4_139_fulltext_tags.json index 5e234d2..4049a8b 100644 --- a/tests/stubdata/output/jats_aj_158_4_139_fulltext_tags.json +++ b/tests/stubdata/output/jats_aj_158_4_139_fulltext_tags.json @@ -1,3 +1,14 @@ -{"unresolved": {"ajab3643bib21": ["

Fortuitously, the timing of the ALMA observations [...] The last full fade and revival cycle of the SEB took place in 20092011 (Fletcher et al. 2011, 2017a), where the word fading is used when the SEB loses its brown color and turns white [...]

"], -"ajab3643bib22": ["

Fortuitously, the timing of the ALMA observations [...] The last full fade and revival cycle of the SEB took place in 20092011 (Fletcher et al. 2011, 2017a), where the word fading is used when the SEB loses its brown color and turns white [...]

", "

ALMA observed Jupiter just a few days after an outbreak [...] The event shows a strong resemblance with the SEB revival in 20102011 (Fletcher et al. 2017a), a series of convective events [...]

", "

At mid-IR wavelengths [...] Such a stratospheric thermal wave was clearly present during the 20102011 SEB revival (Fletcher et al. 2017a).

", "

Fletcher et al. (2017a) compared the convective eruptions triggering the 20102011 SEB revival with mesoscale convective storms (MCS) seen on Earth [...]

"]}, -"resolved": {}} +{ + "resolved": {}, + "unresolved": { + "ajab3643bib21": [ + "

Fortuitously, the timing of the ALMA observations [...] The last full fade and revival cycle of the SEB took place in 20092011 (Fletcher et al. 2011, 2017a), where the word fading is used when the SEB loses its brown color and turns white [...]

" + ], + "ajab3643bib22": [ + "

Fortuitously, the timing of the ALMA observations [...] The last full fade and revival cycle of the SEB took place in 20092011 (Fletcher et al. 2011, 2017a), where the word fading is used when the SEB loses its brown color and turns white [...]

", + "

ALMA observed Jupiter just a few days after an outbreak [...] The event shows a strong resemblance with the SEB revival in 20102011 (Fletcher et al. 2017a), a series of convective events [...]

", + "

At mid-IR wavelengths [...] Such a stratospheric thermal wave was clearly present during the 20102011 SEB revival (Fletcher et al. 2017a).

", + "

Fletcher et al. (2017a) compared the convective eruptions triggering the 20102011 SEB revival with mesoscale convective storms (MCS) seen on Earth [...]

" + ] + } +} diff --git a/tests/stubdata/output/jats_iop_aj_162_1.json b/tests/stubdata/output/jats_iop_aj_162_1.json index e56ce4d..b524798 100644 --- a/tests/stubdata/output/jats_iop_aj_162_1.json +++ b/tests/stubdata/output/jats_iop_aj_162_1.json @@ -1,103 +1,151 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" + "abstract": { + "textEnglish": "We answer the question of whether long-period comet C/1961 T1 (Seki) is the parent body of a meteor shower observed in Earth\u2019s atmosphere. We model discrete parts of a meteoroid stream associated with this comet and follow the orbital evolution of its particles via a numerical integration of their orbits. The gravitational perturbations of major planets and the Poynting\u2013Robertson effect, which influences the motion of the particles, are taken into account. We predict two showers which are related to C/1961 T1. One of these showers was identified with the December &rgr;-Virginids, #502. This identification confirms an earlier suggested relationship between the shower and the comet. The second predicted shower was identified with the \u03b3-Sagittariids, #657. The radiant areas of both showers are symmetrical in respect to the apex of Earth\u2019s heliocentric motion." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "ajabfdc9af1", + "affPubRaw": "Astronomical Institute, Slovak Academy of Science, 05960 Tatransk\u00e1 Lomnica, Slovakia" + } + ], + "attrib": { + "email": "ne@ta3.sk", + "orcid": "0000-0001-9758-1144" + }, + "name": { + "given_name": "Lubo\u0161", + "surname": "Neslu\u0161an" + } + }, + { + "affiliation": [ + { + "affPubID": "ajabfdc9af2", + "affPubRaw": "Astronomical Institute, Slovak Academy of Science, D\u00fabravsk\u00e1 cesta 9, 84504 Bratislava, Slovakia" + } + ], + "attrib": { + "orcid": "0000-0002-7837-2627" + }, + "name": { + "given_name": "M\u00e1ria", + "surname": "Hajdukov\u00e1" + } + } + ], + "copyright": { + "statement": "\u00a9 2021. The American Astronomical Society. All rights reserved.", + "status": true }, "editorialHistory": { + "acceptedDate": "2021-05-02", "receivedDates": [ "2020-12-17" ], "revisedDates": [ "2021-02-08" - ], - "acceptedDate": "2021-05-02" - }, - "pubDate": { - "electrDate": "2021-06-18", - "printDate": "2021-07-00" - }, - "publication": { - "pubName": "The Astronomical Journal", - "publisher": "The American Astronomical Society", - "issueNum": "1", - "volumeNum": "162", - "pubYear": "2021", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "0004-6256" - }, - { - "pubtype": "epub", - "issnString": "1538-3881" - } ] }, - "persistentIDs": [ + "funding": [ { - "DOI": "10.3847/1538-3881/abfdc9" + "agencyid": { + "idschema": "doi", + "idvalue": "https://doi.org/10.13039/501100008530" + }, + "agencyname": "EC ∣ European Regional Development Fund (ERDF)\n", + "awardnumber": "ITMS 26230120002" + }, + { + "agencyname": "Slovak Research and Development Agency", + "awardnumber": "APVV-16-0148" + }, + { + "agencyname": "Slovak Grant Agency for Science, VEGA", + "awardnumber": "2/0037/18" } ], - "publisherIDs": [ + "keywords": [ + { + "keyID": "280", + "keyString": "Comets", + "keySystem": "UAT" + }, + { + "keyID": "1035", + "keyString": "Meteor streams", + "keySystem": "UAT" + }, + { + "keyID": "1034", + "keyString": "Meteor showers", + "keySystem": "UAT" + }, { - "attribute": "publisher-id", - "Identifier": "ajabfdc9" + "keyString": "Comets", + "keySystem": "AAS" }, { - "attribute": "manuscript", - "Identifier": "abfdc9" + "keyString": "Meteor streams", + "keySystem": "AAS" }, { - "attribute": "other", - "Identifier": "AAS29268" + "keyString": "Meteor showers", + "keySystem": "AAS" } ], "pagination": { - "pageCount": "9", - "electronicID": "20" + "electronicID": "20", + "pageCount": "9" }, - "authors": [ + "persistentIDs": [ { - "name": { - "surname": "Neslu\u0161an", - "given_name": "Lubo\u0161" + "DOI": "10.3847/1538-3881/abfdc9" + } + ], + "pubDate": { + "electrDate": "2021-06-18", + "printDate": "2021-07-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "0004-6256", + "pubtype": "ppub" }, - "affiliation": [ - { - "affPubRaw": "Astronomical Institute, Slovak Academy of Science, 05960 Tatransk\u00e1 Lomnica, Slovakia", - "affPubID": "ajabfdc9af1" - } - ], - "attrib": { - "email": "ne@ta3.sk", - "orcid": "0000-0001-9758-1144" + { + "issnString": "1538-3881", + "pubtype": "epub" } + ], + "issueNum": "1", + "pubName": "The Astronomical Journal", + "pubYear": "2021", + "publisher": "The American Astronomical Society", + "volumeNum": "162" + }, + "publisherIDs": [ + { + "Identifier": "ajabfdc9", + "attribute": "publisher-id" }, { - "name": { - "surname": "Hajdukov\u00e1", - "given_name": "M\u00e1ria" - }, - "affiliation": [ - { - "affPubRaw": "Astronomical Institute, Slovak Academy of Science, D\u00fabravsk\u00e1 cesta 9, 84504 Bratislava, Slovakia", - "affPubID": "ajabfdc9af2" - } - ], - "attrib": { - "orcid": "0000-0002-7837-2627" - } + "Identifier": "abfdc9", + "attribute": "manuscript" + }, + { + "Identifier": "AAS29268", + "attribute": "other" } ], - "title": { - "textEnglish": "Meteoroid Stream of Comet C/1961 T1 (Seki) and Its Relation to the December &rgr;-Virginids and \u03b3-Sagittariids" - }, - "abstract": { - "textEnglish": "We answer the question of whether long-period comet C/1961 T1 (Seki) is the parent body of a meteor shower observed in Earth\u2019s atmosphere. We model discrete parts of a meteoroid stream associated with this comet and follow the orbital evolution of its particles via a numerical integration of their orbits. The gravitational perturbations of major planets and the Poynting\u2013Robertson effect, which influences the motion of the particles, are taken into account. We predict two showers which are related to C/1961 T1. One of these showers was identified with the December &rgr;-Virginids, #502. This identification confirms an earlier suggested relationship between the shower and the comet. The second predicted shower was identified with the \u03b3-Sagittariids, #657. The radiant areas of both showers are symmetrical in respect to the apex of Earth\u2019s heliocentric motion." + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " Abedin A. Spurn\u00fd P. Wiegert P. 2015 Icar 261 100 2015Icar..261..100A 10.1016/j.icarus.2015.08.016 ", @@ -171,55 +219,7 @@ " Younger J. P. Reid I. M. Vincent R. A. Holdsworth D. A. Murphy D. J. 2009 MNRAS 398 350 2009MNRAS.398..350Y 10.1111/j.1365-2966.2009.15142.x ", " Younger J. P. Reid I. M. Vincent R. A. Murphy D. J. 2012 MNRAS 425 1473 2012MNRAS.425.1473Y 10.1111/j.1365-2966.2012.21632.x " ], - "keywords": [ - { - "keyString": "Comets", - "keySystem": "UAT", - "keyID": "280" - }, - { - "keyString": "Meteor streams", - "keySystem": "UAT", - "keyID": "1035" - }, - { - "keyString": "Meteor showers", - "keySystem": "UAT", - "keyID": "1034" - }, - { - "keyString": "Comets", - "keySystem": "AAS" - }, - { - "keyString": "Meteor streams", - "keySystem": "AAS" - }, - { - "keyString": "Meteor showers", - "keySystem": "AAS" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 2021. The American Astronomical Society. All rights reserved." - }, - "funding": [ - { - "agencyname": "EC ∣ European Regional Development Fund (ERDF)\n", - "agencyid": { - "idschema": "doi", - "idvalue": "https://doi.org/10.13039/501100008530" - }, - "awardnumber": "ITMS 26230120002" - }, - { - "agencyname": "Slovak Research and Development Agency", - "awardnumber": "APVV-16-0148" - }, - { - "agencyname": "Slovak Grant Agency for Science, VEGA", - "awardnumber": "2/0037/18" - } - ] + "title": { + "textEnglish": "Meteoroid Stream of Comet C/1961 T1 (Seki) and Its Relation to the December &rgr;-Virginids and \u03b3-Sagittariids" + } } diff --git a/tests/stubdata/output/jats_iop_ansnn_12_2_025001.json b/tests/stubdata/output/jats_iop_ansnn_12_2_025001.json index 1569122..be73c1b 100644 --- a/tests/stubdata/output/jats_iop_ansnn_12_2_025001.json +++ b/tests/stubdata/output/jats_iop_ansnn_12_2_025001.json @@ -1,160 +1,183 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2021-01-21" - ], - "acceptedDate": "2021-03-17" - }, - "pubDate": { - "electrDate": "2021-04-30", - "printDate": "2021-06-00" - }, - "publication": { - "pubName": "Advances in Natural Sciences: Nanoscience and Nanotechnology", - "publisher": "IOP Publishing", - "issueNum": "2", - "volumeNum": "12", - "pubYear": "2021", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "2043-6262" - }, - { - "pubtype": "epub", - "issnString": "2043-6262" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1088/2043-6262/abfa8e" - } - ], - "publisherIDs": [ - { - "attribute": "publisher-id", - "Identifier": "ansnabfa8e" - }, - { - "attribute": "manuscript", - "Identifier": "abfa8e" - }, - { - "attribute": "other", - "Identifier": "ANSN-1225005" - } - ], - "pagination": { - "pageCount": "8", - "electronicID": "025001" + "abstract": { + "textEnglish": "This study presents a high porous nanocomposite composed of reduced graphene oxide and NiMoS4 (RGO/NiMoS4) for supercapacitor electrode materials. The different morphologies of NiMoS4 growth on RGO sheets were obtained via a facile one-step microwave-assisted method. The obtained material comprised NiMoS4 nanoneedles of several nanometers in diameter, which are well attached to the surface of RGO nanosheets. The RGO/NiMoS4 nanocomposite had a mesoporous structure, high specific surface area, and high electric conductivity. These excellent characteristics yield a fast electron and ion transport, and a large number of electroactive sites. The RGO/NiMoS4 composite delivered a specific capacitance of 1273 F g1 at a current density of 1.0 A g1, high-rate capability of 71.3 retention from 1 to 6.5 A g1. Besides, an asymmetric supercapacitor device had a capacitance of 80 F g1 at a current density of 1.0 A g1 and an energy density of 82.5 Wh kg1 at a power density of 1000 W kg1 with an operating voltage of 1.6 V. Thus, the current RGO/NiMoS4 nanocomposite has a great potential for energy storage application." }, "authors": [ { - "name": { - "surname": "Van Hoa", - "given_name": "Nguyen" - }, "affiliation": [ { - "affPubRaw": "Faculty of Food Technology, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam", - "affPubID": "ansnabfa8eaf1" + "affPubID": "ansnabfa8eaf1", + "affPubRaw": "Faculty of Food Technology, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam" }, { - "affPubRaw": "Center for Experiments and Practices, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam", - "affPubID": "ansnabfa8eaf2" + "affPubID": "ansnabfa8eaf2", + "affPubRaw": "Center for Experiments and Practices, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam" } ], "attrib": { "email": "hoadhnt@gmail.com" + }, + "name": { + "given_name": "Nguyen", + "surname": "Van Hoa" } }, { - "name": { - "surname": "Dat", - "given_name": "Pham Anh" - }, "affiliation": [ { - "affPubRaw": "Faculty of Food Technology, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam", - "affPubID": "ansnabfa8eaf1" + "affPubID": "ansnabfa8eaf1", + "affPubRaw": "Faculty of Food Technology, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam" } - ] + ], + "name": { + "given_name": "Pham Anh", + "surname": "Dat" + } }, { - "name": { - "surname": "Ngoc Le", - "given_name": "Tran" - }, "affiliation": [ { - "affPubRaw": "Center for Experiments and Practices, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam", - "affPubID": "ansnabfa8eaf2" + "affPubID": "ansnabfa8eaf2", + "affPubRaw": "Center for Experiments and Practices, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam" } - ] + ], + "name": { + "given_name": "Tran", + "surname": "Ngoc Le" + } }, { - "name": { - "surname": "Minh", - "given_name": "Nguyen Cong" - }, "affiliation": [ { - "affPubRaw": "Institute of Biotechnology and Environment, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam", - "affPubID": "ansnabfa8eaf3" + "affPubID": "ansnabfa8eaf3", + "affPubRaw": "Institute of Biotechnology and Environment, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam" } - ] + ], + "name": { + "given_name": "Nguyen Cong", + "surname": "Minh" + } }, { - "name": { - "surname": "Van Tang", - "given_name": "Nguyen" - }, "affiliation": [ { - "affPubRaw": "Faculty of Food Technology, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam", - "affPubID": "ansnabfa8eaf1" + "affPubID": "ansnabfa8eaf1", + "affPubRaw": "Faculty of Food Technology, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam" } - ] + ], + "name": { + "given_name": "Nguyen", + "surname": "Van Tang" + } }, { - "name": { - "surname": "Thi Nga", - "given_name": "Dao" - }, "affiliation": [ { - "affPubRaw": "Center for Experiments and Practices, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam", - "affPubID": "ansnabfa8eaf2" + "affPubID": "ansnabfa8eaf2", + "affPubRaw": "Center for Experiments and Practices, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam" } - ] + ], + "name": { + "given_name": "Dao", + "surname": "Thi Nga" + } }, { - "name": { - "surname": "Ngoc", - "given_name": "Tran Quang" - }, "affiliation": [ { - "affPubRaw": "Faculty of Food Technology, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam", - "affPubID": "ansnabfa8eaf1" + "affPubID": "ansnabfa8eaf1", + "affPubRaw": "Faculty of Food Technology, Nha Trang University, 2 Nguyen Dinh Chieu, Nha Trang, Vietnam" } - ] + ], + "name": { + "given_name": "Tran Quang", + "surname": "Ngoc" + } } ], - "title": { - "textEnglish": "Highly porous nanocomposite of NiMoS4 nanosheets and reduced graphene oxide for energy storage application" + "copyright": { + "statement": "2021 Vietnam Academy of Science & Technology", + "status": true }, - "abstract": { - "textEnglish": "This study presents a high porous nanocomposite composed of reduced graphene oxide and NiMoS4 (RGO/NiMoS4) for supercapacitor electrode materials. The different morphologies of NiMoS4 growth on RGO sheets were obtained via a facile one-step microwave-assisted method. The obtained material comprised NiMoS4 nanoneedles of several nanometers in diameter, which are well attached to the surface of RGO nanosheets. The RGO/NiMoS4 nanocomposite had a mesoporous structure, high specific surface area, and high electric conductivity. These excellent characteristics yield a fast electron and ion transport, and a large number of electroactive sites. The RGO/NiMoS4 composite delivered a specific capacitance of 1273 F g1 at a current density of 1.0 A g1, high-rate capability of 71.3 retention from 1 to 6.5 A g1. Besides, an asymmetric supercapacitor device had a capacitance of 80 F g1 at a current density of 1.0 A g1 and an energy density of 82.5 Wh kg1 at a power density of 1000 W kg1 with an operating voltage of 1.6 V. Thus, the current RGO/NiMoS4 nanocomposite has a great potential for energy storage application." + "editorialHistory": { + "acceptedDate": "2021-03-17", + "receivedDates": [ + "2021-01-21" + ] + }, + "keywords": [ + { + "keyString": "supercapacitor", + "keySystem": "misc" + }, + { + "keyString": "graphene", + "keySystem": "misc" + }, + { + "keyString": "molybdate sulfide", + "keySystem": "misc" + }, + { + "keyString": "Nickel sulfide", + "keySystem": "misc" + }, + { + "keyString": "Classification numbers: 2.00, 2.04, 4.00, 5.11, 515", + "keySystem": "misc" + } + ], + "pagination": { + "electronicID": "025001", + "pageCount": "8" + }, + "persistentIDs": [ + { + "DOI": "10.1088/2043-6262/abfa8e" + } + ], + "pubDate": { + "electrDate": "2021-04-30", + "printDate": "2021-06-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "2043-6262", + "pubtype": "ppub" + }, + { + "issnString": "2043-6262", + "pubtype": "epub" + } + ], + "issueNum": "2", + "pubName": "Advances in Natural Sciences: Nanoscience and Nanotechnology", + "pubYear": "2021", + "publisher": "IOP Publishing", + "volumeNum": "12" + }, + "publisherIDs": [ + { + "Identifier": "ansnabfa8e", + "attribute": "publisher-id" + }, + { + "Identifier": "abfa8e", + "attribute": "manuscript" + }, + { + "Identifier": "ANSN-1225005", + "attribute": "other" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " Kumar S Saeed G Zhu L Hui K N Kim N H Lee J H 2021 Chem. Eng. J. 403 115352 10.1016/j.cej.2020.126352 ", @@ -183,30 +206,7 @@ " Han X Tao K Wang D Han L 2018 Nanoscale 10 2735 10.1039/C7NR07931A ", " Hoa N V Dat P A Nghia N H 2021 J. Mater. Sci. 56 5132 10.1007/s10853-020-05591-6 " ], - "keywords": [ - { - "keyString": "supercapacitor", - "keySystem": "misc" - }, - { - "keyString": "graphene", - "keySystem": "misc" - }, - { - "keyString": "molybdate sulfide", - "keySystem": "misc" - }, - { - "keyString": "Nickel sulfide", - "keySystem": "misc" - }, - { - "keyString": "Classification numbers: 2.00, 2.04, 4.00, 5.11, 515", - "keySystem": "misc" - } - ], - "copyright": { - "status": true, - "statement": "2021 Vietnam Academy of Science & Technology" + "title": { + "textEnglish": "Highly porous nanocomposite of NiMoS4 nanosheets and reduced graphene oxide for energy storage application" } } diff --git a/tests/stubdata/output/jats_iop_apj_923_1_47.json b/tests/stubdata/output/jats_iop_apj_923_1_47.json index 3c48d5e..0a3f3db 100644 --- a/tests/stubdata/output/jats_iop_apj_923_1_47.json +++ b/tests/stubdata/output/jats_iop_apj_923_1_47.json @@ -1,169 +1,215 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2021-04-30" - ], - "revisedDates": [ - "2021-09-07" - ], - "acceptedDate": "2021-09-08" - }, - "pubDate": { - "electrDate": "2021-12-09", - "printDate": "2021-12-00" - }, - "publication": { - "pubName": "The Astrophysical Journal", - "publisher": "The American Astronomical Society", - "issueNum": "1", - "volumeNum": "923", - "pubYear": "2021", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "0004-637X" - }, - { - "pubtype": "epub", - "issnString": "1538-4357" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.3847/1538-4357/ac25ea" - } - ], - "publisherIDs": [ - { - "attribute": "publisher-id", - "Identifier": "apjac25ea" - }, - { - "attribute": "manuscript", - "Identifier": "ac25ea" - }, - { - "attribute": "other", - "Identifier": "AAS31921" - } - ], - "pagination": { - "pageCount": "14", - "electronicID": "47" + "abstract": { + "textEnglish": "Radioactive nuclei were present in the early solar system (ESS), as inferred from analysis of meteorites. Many are produced in massive stars, either during their lives or their final explosions. In the first paper of this series (Brinkman et al. 2019), we focused on the production of 26Al in massive binaries. Here, we focus on the production of another two short-lived radioactive nuclei, 36Cl and 41Ca, and the comparison to the ESS data. We used the MESA stellar evolution code with an extended nuclear network and computed massive (10\u201380 M \u2299), rotating (with initial velocities of 150 and 300 km s\u22121) and nonrotating single stars at solar metallicity (Z = 0.014) up to the onset of core collapse. We present the wind yields for the radioactive isotopes 26Al, 36Cl, and 41Ca, and the stable isotopes 19F and 22Ne. In relation to the stable isotopes, we find that only the most massive models, \u226560 and \u226540 M \u2299 give positive 19F and 22Ne yields, respectively, depending on the initial rotation rate. In relation to the radioactive isotopes, we find that the ESS abundances of 26Al and 41Ca can be matched with by models with initial masses \u226540 M \u2299, while 36Cl is matched only by our most massive models, \u226560 M \u2299. 60Fe is not significantly produced by any wind model, as required by the observations. Therefore, massive star winds are a favored candidate for the origin of the very short-lived 26Al, 36Cl, and 41Ca in the ESS." }, "authors": [ { - "name": { - "surname": "Brinkman", - "given_name": "Hannah E." - }, "affiliation": [ { - "affPubRaw": "Konkoly Observatory, Research Centre for Astronomy and Earth Sciences (CSFK), E\u00f6tv\u00f6s Lor\u00e1nd Research Network (ELKH), Konkoly Thege Mikl\u00f3s \u00fat 15-17, H-1121 Budapest, Hungary", - "affPubID": "affiliation01" + "affPubID": "affiliation01", + "affPubRaw": "Konkoly Observatory, Research Centre for Astronomy and Earth Sciences (CSFK), E\u00f6tv\u00f6s Lor\u00e1nd Research Network (ELKH), Konkoly Thege Mikl\u00f3s \u00fat 15-17, H-1121 Budapest, Hungary" }, { - "affPubRaw": "Graduate School of Physics, University of Szeged, Dom t\u00e9r 9, Szeged, 6720 Hungary", - "affPubID": "affiliation02" + "affPubID": "affiliation02", + "affPubRaw": "Graduate School of Physics, University of Szeged, Dom t\u00e9r 9, Szeged, 6720 Hungary" } ], "attrib": { "email": "hannah.brinkman@csfk.org" + }, + "name": { + "given_name": "Hannah E.", + "surname": "Brinkman" } }, { - "name": { - "surname": "Hartogh", - "given_name": "J. W. den" - }, "affiliation": [ { - "affPubRaw": "Konkoly Observatory, Research Centre for Astronomy and Earth Sciences (CSFK), E\u00f6tv\u00f6s Lor\u00e1nd Research Network (ELKH), Konkoly Thege Mikl\u00f3s \u00fat 15-17, H-1121 Budapest, Hungary", - "affPubID": "affiliation01" + "affPubID": "affiliation01", + "affPubRaw": "Konkoly Observatory, Research Centre for Astronomy and Earth Sciences (CSFK), E\u00f6tv\u00f6s Lor\u00e1nd Research Network (ELKH), Konkoly Thege Mikl\u00f3s \u00fat 15-17, H-1121 Budapest, Hungary" } - ] + ], + "name": { + "given_name": "J. W. den", + "surname": "Hartogh" + } }, { - "name": { - "surname": "Doherty", - "given_name": "C. L." - }, "affiliation": [ { - "affPubRaw": "Konkoly Observatory, Research Centre for Astronomy and Earth Sciences (CSFK), E\u00f6tv\u00f6s Lor\u00e1nd Research Network (ELKH), Konkoly Thege Mikl\u00f3s \u00fat 15-17, H-1121 Budapest, Hungary", - "affPubID": "affiliation01" + "affPubID": "affiliation01", + "affPubRaw": "Konkoly Observatory, Research Centre for Astronomy and Earth Sciences (CSFK), E\u00f6tv\u00f6s Lor\u00e1nd Research Network (ELKH), Konkoly Thege Mikl\u00f3s \u00fat 15-17, H-1121 Budapest, Hungary" }, { - "affPubRaw": "School of Physics and Astronomy, Monash University, VIC 3800, Australia", - "affPubID": "affiliation03" + "affPubID": "affiliation03", + "affPubRaw": "School of Physics and Astronomy, Monash University, VIC 3800, Australia" } - ] + ], + "name": { + "given_name": "C. L.", + "surname": "Doherty" + } }, { - "name": { - "surname": "Pignatari", - "given_name": "M." - }, "affiliation": [ { - "affPubRaw": "Konkoly Observatory, Research Centre for Astronomy and Earth Sciences (CSFK), E\u00f6tv\u00f6s Lor\u00e1nd Research Network (ELKH), Konkoly Thege Mikl\u00f3s \u00fat 15-17, H-1121 Budapest, Hungary", - "affPubID": "affiliation01" + "affPubID": "affiliation01", + "affPubRaw": "Konkoly Observatory, Research Centre for Astronomy and Earth Sciences (CSFK), E\u00f6tv\u00f6s Lor\u00e1nd Research Network (ELKH), Konkoly Thege Mikl\u00f3s \u00fat 15-17, H-1121 Budapest, Hungary" }, { - "affPubRaw": "E.A. Milne Centre for Astrophysics, Department of Physics and Mathematics, University of Hull, HU6 7RX, UK", - "affPubID": "affiliation04" + "affPubID": "affiliation04", + "affPubRaw": "E.A. Milne Centre for Astrophysics, Department of Physics and Mathematics, University of Hull, HU6 7RX, UK" }, { - "affPubRaw": "NuGrid Collaboration, http://nugridstars.org", - "affPubID": "affiliation05" + "affPubID": "affiliation05", + "affPubRaw": "NuGrid Collaboration, http://nugridstars.org" }, { - "affPubRaw": "Joint Institute for Nuclear Astrophysics, Center for the Evolution of the Elements, Michigan State University, 640 South Shaw Lane, East Lansing, MI 48824, USA", - "affPubID": "affiliation06" + "affPubID": "affiliation06", + "affPubRaw": "Joint Institute for Nuclear Astrophysics, Center for the Evolution of the Elements, Michigan State University, 640 South Shaw Lane, East Lansing, MI 48824, USA" } ], "attrib": { "orcid": "0000-0002-9048-6010" + }, + "name": { + "given_name": "M.", + "surname": "Pignatari" } }, { - "name": { - "surname": "Lugaro", - "given_name": "M." - }, "affiliation": [ { - "affPubRaw": "Konkoly Observatory, Research Centre for Astronomy and Earth Sciences (CSFK), E\u00f6tv\u00f6s Lor\u00e1nd Research Network (ELKH), Konkoly Thege Mikl\u00f3s \u00fat 15-17, H-1121 Budapest, Hungary", - "affPubID": "affiliation01" + "affPubID": "affiliation01", + "affPubRaw": "Konkoly Observatory, Research Centre for Astronomy and Earth Sciences (CSFK), E\u00f6tv\u00f6s Lor\u00e1nd Research Network (ELKH), Konkoly Thege Mikl\u00f3s \u00fat 15-17, H-1121 Budapest, Hungary" }, { - "affPubRaw": "School of Physics and Astronomy, Monash University, VIC 3800, Australia", - "affPubID": "affiliation03" + "affPubID": "affiliation03", + "affPubRaw": "School of Physics and Astronomy, Monash University, VIC 3800, Australia" }, { - "affPubRaw": "ELTE E\u00f6tv\u00f6s Lor\u00e1nd University, Institute of Physics, Budapest 1117, P\u00e1zm\u00e1ny P\u00e9ter s\u00e9t\u00e1ny 1/A, Hungary", - "affPubID": "affiliation07" + "affPubID": "affiliation07", + "affPubRaw": "ELTE E\u00f6tv\u00f6s Lor\u00e1nd University, Institute of Physics, Budapest 1117, P\u00e1zm\u00e1ny P\u00e9ter s\u00e9t\u00e1ny 1/A, Hungary" } ], "attrib": { "orcid": "0000-0002-6972-3958" + }, + "name": { + "given_name": "M.", + "surname": "Lugaro" } } ], - "title": { - "textEnglish": "26Aluminum from Massive Binary Stars. II. Rotating Single Stars Up to Core Collapse and Their Impact on the Early Solar System" + "copyright": { + "statement": "\u00a9 2021. The American Astronomical Society. All rights reserved.", + "status": true }, - "abstract": { - "textEnglish": "Radioactive nuclei were present in the early solar system (ESS), as inferred from analysis of meteorites. Many are produced in massive stars, either during their lives or their final explosions. In the first paper of this series (Brinkman et al. 2019), we focused on the production of 26Al in massive binaries. Here, we focus on the production of another two short-lived radioactive nuclei, 36Cl and 41Ca, and the comparison to the ESS data. We used the MESA stellar evolution code with an extended nuclear network and computed massive (10\u201380 M \u2299), rotating (with initial velocities of 150 and 300 km s\u22121) and nonrotating single stars at solar metallicity (Z = 0.014) up to the onset of core collapse. We present the wind yields for the radioactive isotopes 26Al, 36Cl, and 41Ca, and the stable isotopes 19F and 22Ne. In relation to the stable isotopes, we find that only the most massive models, \u226560 and \u226540 M \u2299 give positive 19F and 22Ne yields, respectively, depending on the initial rotation rate. In relation to the radioactive isotopes, we find that the ESS abundances of 26Al and 41Ca can be matched with by models with initial masses \u226540 M \u2299, while 36Cl is matched only by our most massive models, \u226560 M \u2299. 60Fe is not significantly produced by any wind model, as required by the observations. Therefore, massive star winds are a favored candidate for the origin of the very short-lived 26Al, 36Cl, and 41Ca in the ESS." + "editorialHistory": { + "acceptedDate": "2021-09-08", + "receivedDates": [ + "2021-04-30" + ], + "revisedDates": [ + "2021-09-07" + ] + }, + "funding": [ + { + "agencyid": { + "idschema": "doi", + "idvalue": "https://doi.org/10.13039/501100000781" + }, + "agencyname": "EC \u2223 European Research Council (ERC)\n", + "awardnumber": "724560" + } + ], + "keywords": [ + { + "keyID": "1636", + "keyString": "Stellar winds", + "keySystem": "UAT" + }, + { + "keyID": "1599", + "keyString": "Stellar evolution", + "keySystem": "UAT" + }, + { + "keyID": "1616", + "keyString": "Stellar nucleosynthesis", + "keySystem": "UAT" + }, + { + "keyID": "1528", + "keyString": "Solar system", + "keySystem": "UAT" + }, + { + "keyID": "732", + "keyString": "Massive stars", + "keySystem": "UAT" + }, + { + "keyID": "1629", + "keyString": "Stellar rotation", + "keySystem": "UAT" + } + ], + "openAccess": { + "license": "This article is available under the terms of the IOP-Standard License." + }, + "pagination": { + "electronicID": "47", + "pageCount": "14" + }, + "persistentIDs": [ + { + "DOI": "10.3847/1538-4357/ac25ea" + } + ], + "pubDate": { + "electrDate": "2021-12-09", + "printDate": "2021-12-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "0004-637X", + "pubtype": "ppub" + }, + { + "issnString": "1538-4357", + "pubtype": "epub" + } + ], + "issueNum": "1", + "pubName": "The Astrophysical Journal", + "pubYear": "2021", + "publisher": "The American Astronomical Society", + "volumeNum": "923" + }, + "publisherIDs": [ + { + "Identifier": "apjac25ea", + "attribute": "publisher-id" + }, + { + "Identifier": "ac25ea", + "attribute": "manuscript" + }, + { + "Identifier": "AAS31921", + "attribute": "other" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " AbiaC. CristalloS. CunhaK. de LavernyP. SmithV. V. 2019A&A625A402019A&A...625A..40A10.1051/0004-6361/201935286", @@ -249,53 +295,7 @@ " WasserburgG. J. BussoM. GallinoR. NollettK. M. 2006NuPhA77752006NuPhA.777....5W10.1016/j.nuclphysa.2005.07.015", " YoungE. D. 2014E&PSL392162014E&PSL.392...16Y10.1016/j.epsl.2014.02.014" ], - "keywords": [ - { - "keyString": "Stellar winds", - "keySystem": "UAT", - "keyID": "1636" - }, - { - "keyString": "Stellar evolution", - "keySystem": "UAT", - "keyID": "1599" - }, - { - "keyString": "Stellar nucleosynthesis", - "keySystem": "UAT", - "keyID": "1616" - }, - { - "keyString": "Solar system", - "keySystem": "UAT", - "keyID": "1528" - }, - { - "keyString": "Massive stars", - "keySystem": "UAT", - "keyID": "732" - }, - { - "keyString": "Stellar rotation", - "keySystem": "UAT", - "keyID": "1629" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 2021. The American Astronomical Society. All rights reserved." - }, - "openAccess": { - "license": "This article is available under the terms of the IOP-Standard License." - }, - "funding": [ - { - "agencyname": "EC \u2223 European Research Council (ERC)\n", - "agencyid": { - "idschema": "doi", - "idvalue": "https://doi.org/10.13039/501100000781" - }, - "awardnumber": "724560" - } - ] + "title": { + "textEnglish": "26Aluminum from Massive Binary Stars. II. Rotating Single Stars Up to Core Collapse and Their Impact on the Early Solar System" + } } diff --git a/tests/stubdata/output/jats_iop_no_contribs.json b/tests/stubdata/output/jats_iop_no_contribs.json index d0a237d..5e27b58 100644 --- a/tests/stubdata/output/jats_iop_no_contribs.json +++ b/tests/stubdata/output/jats_iop_no_contribs.json @@ -1,72 +1,72 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" + "copyright": { + "statement": "Copyright \u00a9 EPLA, 2023", + "status": true }, "editorialHistory": { + "acceptedDate": "2023-04-25", "receivedDates": [ "2023-04-25" - ], - "acceptedDate": "2023-04-25" + ] + }, + "openAccess": { + "license": "This article is available under the terms of the IOP-Standard License.", + "licenseURL": "https://publishingsupport.iopscience.iop.org/iop-standard/v1" }, + "pagination": { + "electronicID": "30000", + "pageCount": "2" + }, + "persistentIDs": [ + { + "DOI": "10.1209/0295-5075/acd024" + } + ], "pubDate": { "electrDate": "2023-05-02", "printDate": "2023-05-01" }, "publication": { - "pubName": "Europhysics Letters", - "publisher": "EDP Sciences, IOP Publishing and Societ\u00e0 Italiana di Fisica", - "issueNum": "3", - "volumeNum": "142", - "pubYear": "2023", "ISSN": [ { - "pubtype": "ppub", - "issnString": "0295-5075" + "issnString": "0295-5075", + "pubtype": "ppub" }, { - "pubtype": "epub", - "issnString": "1286-4854" + "issnString": "1286-4854", + "pubtype": "epub" } - ] + ], + "issueNum": "3", + "pubName": "Europhysics Letters", + "pubYear": "2023", + "publisher": "EDP Sciences, IOP Publishing and Societ\u00e0 Italiana di Fisica", + "volumeNum": "142" }, - "persistentIDs": [ - { - "DOI": "10.1209/0295-5075/acd024" - } - ], "publisherIDs": [ { - "attribute": "publisher-id", - "Identifier": "epl23100304" + "Identifier": "epl23100304", + "attribute": "publisher-id" }, { - "attribute": "manuscript", - "Identifier": "acd024" + "Identifier": "acd024", + "attribute": "manuscript" } ], - "pagination": { - "pageCount": "2", - "electronicID": "30000" - }, - "title": { - "textEnglish": "Editorial \u2014How to write a good letter for EPL" + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " LetchfordAdrian Moat HelenSusannah PreisTobias 2015R. Soc. Open Sci.2150266", " LiKun 2019EPL12838002", " YangMu LiuHaitao 2022EPL13961002" ], - "copyright": { - "status": true, - "statement": "Copyright \u00a9 EPLA, 2023" - }, - "openAccess": { - "license": "This article is available under the terms of the IOP-Standard License.", - "licenseURL": "https://publishingsupport.iopscience.iop.org/iop-standard/v1" + "title": { + "textEnglish": "Editorial \u2014How to write a good letter for EPL" } } diff --git a/tests/stubdata/output/jats_iop_no_orcid_tag.json b/tests/stubdata/output/jats_iop_no_orcid_tag.json index 10b034b..b3a46fb 100644 --- a/tests/stubdata/output/jats_iop_no_orcid_tag.json +++ b/tests/stubdata/output/jats_iop_no_orcid_tag.json @@ -1,5829 +1,5867 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2022-10-11" - ], - "revisedDates": [ - "2022-11-21" - ], - "acceptedDate": "2022-11-21" - }, - "pubDate": { - "electrDate": "2023-02-07", - "printDate": "2023-02-01" - }, - "publication": { - "pubName": "The Astrophysical Journal Supplement Series", - "publisher": "The American Astronomical Society", - "issueNum": "2", - "volumeNum": "264", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "0067-0049" - }, - { - "pubtype": "epub", - "issnString": "1538-4365" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.3847/1538-4365/aca537" - } - ], - "publisherIDs": [ - { - "attribute": "publisher-id", - "Identifier": "apjsaca537" - }, - { - "attribute": "manuscript", - "Identifier": "aca537" - }, - { - "attribute": "other", - "Identifier": "AAS42590" - } - ], - "pagination": { - "pageCount": "24", - "electronicID": "50" + "abstract": { + "textEnglish": "A catalog containing details of the highest-energy cosmic rays recorded through the detection of extensive air showers at the Pierre Auger Observatory is presented with the aim of opening the data to detailed examination. Descriptions of the 100 showers created by the highest-energy particles recorded between 2004 January 1 and 2020 December 31 are given for cosmic rays that have energies in the range 78\u2013166 EeV. Details are also given on a further nine very energetic events that have been used in the calibration procedure adopted to determine the energy of each primary. A sky plot of the arrival directions of the most energetic particles is shown. No interpretations of the data are offered." }, "authors": [ { - "name": { - "surname": "Abdul Halim", - "given_name": "A." - }, "affiliation": [ { - "affPubRaw": "University of Adelaide, Adelaide, SA, Australia", - "affPubID": "affiliation01" + "affPubID": "affiliation01", + "affPubRaw": "University of Adelaide, Adelaide, SA, Australia" } ], "attrib": { "orcid": "0000-0003-1218-1737" + }, + "name": { + "given_name": "A.", + "surname": "Abdul Halim" } }, { - "name": { - "surname": "Abreu", - "given_name": "P." - }, "affiliation": [ { - "affPubRaw": "Laborat\u00f3rio de Instrumenta\u00e7\u00e3o e F\u00edsica Experimental de Part\u00edculas (LIP) and Instituto Superior T\u00e9cnico (IST), Universidade de Lisboa (UL), Lisboa, Portugal", - "affPubID": "affiliation02" + "affPubID": "affiliation02", + "affPubRaw": "Laborat\u00f3rio de Instrumenta\u00e7\u00e3o e F\u00edsica Experimental de Part\u00edculas (LIP) and Instituto Superior T\u00e9cnico (IST), Universidade de Lisboa (UL), Lisboa, Portugal" } ], "attrib": { "orcid": "0000-0002-9973-7314" + }, + "name": { + "given_name": "P.", + "surname": "Abreu" } }, { - "name": { - "surname": "Aglietta", - "given_name": "M." - }, "affiliation": [ { - "affPubRaw": "INFN, Sezione di Torino, Torino, Italy", - "affPubID": "affiliation03" + "affPubID": "affiliation03", + "affPubRaw": "INFN, Sezione di Torino, Torino, Italy" }, { - "affPubRaw": "Osservatorio Astrofisico di Torino (INAF), Torino, Italy", - "affPubID": "affiliation04" + "affPubID": "affiliation04", + "affPubRaw": "Osservatorio Astrofisico di Torino (INAF), Torino, Italy" } ], "attrib": { "orcid": "0000-0001-8354-5388" + }, + "name": { + "given_name": "M.", + "surname": "Aglietta" } }, { - "name": { - "surname": "Allekotte", - "given_name": "I." - }, "affiliation": [ { - "affPubRaw": "Centro At\u00f3mico Bariloche and Instituto Balseiro (CNEA-UNCuyo-CONICET), San Carlos de Bariloche, Argentina", - "affPubID": "affiliation05" + "affPubID": "affiliation05", + "affPubRaw": "Centro At\u00f3mico Bariloche and Instituto Balseiro (CNEA-UNCuyo-CONICET), San Carlos de Bariloche, Argentina" } ], "attrib": { "orcid": "0000-0002-9624-3044" + }, + "name": { + "given_name": "I.", + "surname": "Allekotte" } }, { - "name": { - "surname": "Allison", - "given_name": "P." - }, "affiliation": [ { - "affPubRaw": "Ohio State University, Columbus, OH, USA", - "affPubID": "affiliation06" + "affPubID": "affiliation06", + "affPubRaw": "Ohio State University, Columbus, OH, USA" } - ] + ], + "name": { + "given_name": "P.", + "surname": "Allison" + } }, { - "name": { - "surname": "Almeida Cheminant", - "given_name": "K." - }, "affiliation": [ { - "affPubRaw": "Institute of Nuclear Physics PAN, Krakow, Poland", - "affPubID": "affiliation07" + "affPubID": "affiliation07", + "affPubRaw": "Institute of Nuclear Physics PAN, Krakow, Poland" } ], "attrib": { "orcid": "0000-0001-6352-5339" + }, + "name": { + "given_name": "K.", + "surname": "Almeida Cheminant" } }, { - "name": { - "surname": "Almela", - "given_name": "A." - }, "affiliation": [ { - "affPubRaw": "Instituto de Tecnolog\u00edas en Detecci\u00f3n y Astropart\u00edculas (CNEA, CONICET, UNSAM), Buenos Aires, Argentina", - "affPubID": "affiliation08" + "affPubID": "affiliation08", + "affPubRaw": "Instituto de Tecnolog\u00edas en Detecci\u00f3n y Astropart\u00edculas (CNEA, CONICET, UNSAM), Buenos Aires, Argentina" }, { - "affPubRaw": "Universidad Tecnol\u00f3gica Nacional\u2014Facultad Regional Buenos Aires, Buenos Aires, Argentina", - "affPubID": "affiliation09" + "affPubID": "affiliation09", + "affPubRaw": "Universidad Tecnol\u00f3gica Nacional\u2014Facultad Regional Buenos Aires, Buenos Aires, Argentina" } ], "attrib": { "orcid": "0000-0003-1233-2670" + }, + "name": { + "given_name": "A.", + "surname": "Almela" } }, { - "name": { - "surname": "Alvarez-Mu\u00f1iz", - "given_name": "J." - }, "affiliation": [ { - "affPubRaw": "Instituto Galego de F\u00edsica de Altas Enerx\u00edas (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain", - "affPubID": "affiliation10" + "affPubID": "affiliation10", + "affPubRaw": "Instituto Galego de F\u00edsica de Altas Enerx\u00edas (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain" } ], "attrib": { "orcid": "0000-0002-2367-0803" + }, + "name": { + "given_name": "J.", + "surname": "Alvarez-Mu\u00f1iz" } }, { - "name": { - "surname": "Ammerman Yebra", - "given_name": "J." - }, "affiliation": [ { - "affPubRaw": "Instituto Galego de F\u00edsica de Altas Enerx\u00edas (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain", - "affPubID": "affiliation10" + "affPubID": "affiliation10", + "affPubRaw": "Instituto Galego de F\u00edsica de Altas Enerx\u00edas (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain" } ], "attrib": { "orcid": "0000-0002-2059-6206" + }, + "name": { + "given_name": "J.", + "surname": "Ammerman Yebra" } }, { - "name": { - "surname": "Anastasi", - "given_name": "G. A." - }, "affiliation": [ { - "affPubRaw": "INFN, Sezione di Torino, Torino, Italy", - "affPubID": "affiliation03" + "affPubID": "affiliation03", + "affPubRaw": "INFN, Sezione di Torino, Torino, Italy" }, { - "affPubRaw": "Osservatorio Astrofisico di Torino (INAF), Torino, Italy", - "affPubID": "affiliation04" + "affPubID": "affiliation04", + "affPubRaw": "Osservatorio Astrofisico di Torino (INAF), Torino, Italy" } ], "attrib": { "orcid": "0000-0003-0824-5283" + }, + "name": { + "given_name": "G. 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R." - }, "affiliation": [ { - "affPubRaw": "RWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany", - "affPubID": "affiliation13" + "affPubID": "affiliation13", + "affPubRaw": "RWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany" } ], "attrib": { "orcid": "0000-0002-0502-3602" + }, + "name": { + "given_name": "P. 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A.", + "surname": "Watson" } }, { - "name": { - "surname": "Weindl", - "given_name": "A." - }, "affiliation": [ { - "affPubRaw": "Karlsruhe Institute of Technology (KIT), Institute for Astroparticle Physics, Karlsruhe, Germany", - "affPubID": "affiliation31" + "affPubID": "affiliation31", + "affPubRaw": "Karlsruhe Institute of Technology (KIT), Institute for Astroparticle Physics, Karlsruhe, Germany" } ], "attrib": { "orcid": "0000-0003-4929-6191" + }, + "name": { + "given_name": "A.", + "surname": "Weindl" } }, { - "name": { - "surname": "Wiencke", - "given_name": "L." - }, "affiliation": [ { - "affPubRaw": "Colorado School of Mines, Golden, CO, USA", - "affPubID": "affiliation77" + "affPubID": "affiliation77", + "affPubRaw": "Colorado School of Mines, Golden, CO, USA" } ], "attrib": { "orcid": "0000-0003-2878-9704" + }, + "name": { + "given_name": "L.", + "surname": "Wiencke" } }, { - "name": { - "surname": "Wilczy\u0144ski", - "given_name": "H." - }, "affiliation": [ { - "affPubRaw": "Institute of Nuclear Physics PAN, Krakow, Poland", - "affPubID": "affiliation07" + "affPubID": "affiliation07", + "affPubRaw": "Institute of Nuclear Physics PAN, Krakow, Poland" } ], "attrib": { "orcid": "0000-0003-2652-9685" + }, + "name": { + "given_name": "H.", + "surname": "Wilczy\u0144ski" } }, { - "name": { - "surname": "Wittkowski", - "given_name": "D." - }, "affiliation": [ { - "affPubRaw": "Bergische Universit\u00e4t Wuppertal, Department of Physics, Wuppertal, Germany", - "affPubID": "affiliation46" + "affPubID": "affiliation46", + "affPubRaw": "Bergische Universit\u00e4t Wuppertal, Department of Physics, Wuppertal, Germany" } - ] + ], + "name": { + "given_name": "D.", + "surname": "Wittkowski" + } }, { - "name": { - "surname": "Wundheiler", - "given_name": "B." - }, "affiliation": [ { - "affPubRaw": "Instituto de Tecnolog\u00edas en Detecci\u00f3n y Astropart\u00edculas (CNEA, CONICET, UNSAM), Buenos Aires, Argentina", - "affPubID": "affiliation08" + "affPubID": "affiliation08", + "affPubRaw": "Instituto de Tecnolog\u00edas en Detecci\u00f3n y Astropart\u00edculas (CNEA, CONICET, UNSAM), Buenos Aires, Argentina" } ], "attrib": { "orcid": "0000-0003-3121-7037" + }, + "name": { + "given_name": "B.", + "surname": "Wundheiler" } }, { - "name": { - "surname": "Younk", - "given_name": "P." - }, "affiliation": [ { - "affPubRaw": "Los Alamos National Laboratory, Los Alamos, NM, USA", - "affPubID": "affiliation99" + "affPubID": "affiliation99", + "affPubRaw": "Los Alamos National Laboratory, Los Alamos, NM, USA" } - ] + ], + "name": { + "given_name": "P.", + "surname": "Younk" + } }, { - "name": { - "surname": "Yushkov", - "given_name": "A." - }, "affiliation": [ { - "affPubRaw": "Institute of Physics of the Czech Academy of Sciences, Prague, Czech Republic", - "affPubID": "affiliation21" + "affPubID": "affiliation21", + "affPubRaw": "Institute of Physics of the Czech Academy of Sciences, Prague, Czech Republic" } ], "attrib": { "orcid": "0000-0001-5107-9116" + }, + "name": { + "given_name": "A.", + "surname": "Yushkov" } }, { - "name": { - "surname": "Zapparrata", - "given_name": "O." - }, "affiliation": [ { - "affPubRaw": "Universit\u00e9 Libre de Bruxelles (ULB), Brussels, Belgium", - "affPubID": "affiliation73" + "affPubID": "affiliation73", + "affPubRaw": "Universit\u00e9 Libre de Bruxelles (ULB), Brussels, Belgium" } ], "attrib": { "orcid": "0000-0002-8839-4715" + }, + "name": { + "given_name": "O.", + "surname": "Zapparrata" } }, { - "name": { - "surname": "Zas", - "given_name": "E." - }, "affiliation": [ { - "affPubRaw": "Instituto Galego de F\u00edsica de Altas Enerx\u00edas (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain", - "affPubID": "affiliation10" + "affPubID": "affiliation10", + "affPubRaw": "Instituto Galego de F\u00edsica de Altas Enerx\u00edas (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain" } ], "attrib": { "orcid": "0000-0002-4430-8117" + }, + "name": { + "given_name": "E.", + "surname": "Zas" } }, { - "name": { - "surname": "Zavrtanik", - "given_name": "D." - }, "affiliation": [ { - "affPubRaw": "Center for Astrophysics and Cosmology (CAC), University of Nova Gorica, Nova Gorica, Slovenia", - "affPubID": "affiliation71" + "affPubID": "affiliation71", + "affPubRaw": "Center for Astrophysics and Cosmology (CAC), University of Nova Gorica, Nova Gorica, Slovenia" }, { - "affPubRaw": "Experimental Particle Physics Department, J. Stefan Institute, Ljubljana, Slovenia", - "affPubID": "affiliation72" + "affPubID": "affiliation72", + "affPubRaw": "Experimental Particle Physics Department, J. Stefan Institute, Ljubljana, Slovenia" } ], "attrib": { "orcid": "0000-0002-4596-1521" + }, + "name": { + "given_name": "D.", + "surname": "Zavrtanik" } }, { - "name": { - "surname": "Zavrtanik", - "given_name": "M." - }, "affiliation": [ { - "affPubRaw": "Center for Astrophysics and Cosmology (CAC), University of Nova Gorica, Nova Gorica, Slovenia", - "affPubID": "affiliation71" + "affPubID": "affiliation71", + "affPubRaw": "Center for Astrophysics and Cosmology (CAC), University of Nova Gorica, Nova Gorica, Slovenia" }, { - "affPubRaw": "Experimental Particle Physics Department, J. Stefan Institute, Ljubljana, Slovenia", - "affPubID": "affiliation72" + "affPubID": "affiliation72", + "affPubRaw": "Experimental Particle Physics Department, J. Stefan Institute, Ljubljana, Slovenia" } ], "attrib": { "orcid": "0000-0001-5606-6912" + }, + "name": { + "given_name": "M.", + "surname": "Zavrtanik" } }, { - "name": { - "collab": "(The Pierre Auger Collaboration)" - }, "attrib": { "collab": true + }, + "name": { + "collab": "(The Pierre Auger Collaboration)" } } ], - "title": { - "textEnglish": "A Catalog of the Highest-energy Cosmic Rays Recorded during Phase I of Operation of the Pierre Auger Observatory" + "copyright": { + "statement": "\u00a9 2023. The Author(s). Published by the American Astronomical Society.", + "status": true }, - "abstract": { - "textEnglish": "A catalog containing details of the highest-energy cosmic rays recorded through the detection of extensive air showers at the Pierre Auger Observatory is presented with the aim of opening the data to detailed examination. Descriptions of the 100 showers created by the highest-energy particles recorded between 2004 January 1 and 2020 December 31 are given for cosmic rays that have energies in the range 78\u2013166 EeV. Details are also given on a further nine very energetic events that have been used in the calibration procedure adopted to determine the energy of each primary. A sky plot of the arrival directions of the most energetic particles is shown. No interpretations of the data are offered." + "editorialHistory": { + "acceptedDate": "2022-11-21", + "receivedDates": [ + "2022-10-11" + ], + "revisedDates": [ + "2022-11-21" + ] + }, + "funding": [ + { + "agencyid": { + "idschema": "doi", + "idvalue": "https://doi.org/10.13039/501100003074" + }, + "agencyname": "MINCyT \u2223 Agencia Nacional de Promoci\u00f3n Cient\u00edfica y Tecnol\u00f3gica (ANPCyT)\n", + "awardnumber": "0" + } + ], + "keywords": [ + { + "keyID": "1733", + "keyString": "Ultra-high-energy cosmic radiation", + "keySystem": "UAT" + }, + { + "keyID": "327", + "keyString": "Cosmic ray showers", + "keySystem": "UAT" + }, + { + "keyID": "2371", + "keyString": "Experimental data", + "keySystem": "UAT" + }, + { + "keyID": "205", + "keyString": "Catalogs", + "keySystem": "UAT" + } + ], + "openAccess": { + "license": "\n\nOriginal content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.", + "licenseURL": "http://creativecommons.org/licenses/by/4.0/", + "open": true + }, + "pagination": { + "electronicID": "50", + "pageCount": "24" + }, + "persistentIDs": [ + { + "DOI": "10.3847/1538-4365/aca537" + } + ], + "pubDate": { + "electrDate": "2023-02-07", + "printDate": "2023-02-01" + }, + "publication": { + "ISSN": [ + { + "issnString": "0067-0049", + "pubtype": "ppub" + }, + { + "issnString": "1538-4365", + "pubtype": "epub" + } + ], + "issueNum": "2", + "pubName": "The Astrophysical Journal Supplement Series", + "pubYear": "2023", + "publisher": "The American Astronomical Society", + "volumeNum": "264" + }, + "publisherIDs": [ + { + "Identifier": "apjsaca537", + "attribute": "publisher-id" + }, + { + "Identifier": "aca537", + "attribute": "manuscript" + }, + { + "Identifier": "AAS42590", + "attribute": "other" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " AabA. AbreuP. AgliettaM. 2014aPhRvD901220052014PhRvD..90l2005A10.1103/PhysRevD.90.122005", @@ -5870,45 +5908,7 @@ " Vali\u00f1oI. Alvarez-Mu\u00f1izJ. RothM. VazquezR. A. ZasE. 2010APh323042010APh....32..304V10.1016/j.astropartphys.2009.09.008", " YushkovA. 2019ICRC (Madison)364822019ICRC...36..482Y10.22323/1.358.0482" ], - "keywords": [ - { - "keyString": "Ultra-high-energy cosmic radiation", - "keySystem": "UAT", - "keyID": "1733" - }, - { - "keyString": "Cosmic ray showers", - "keySystem": "UAT", - "keyID": "327" - }, - { - "keyString": "Experimental data", - "keySystem": "UAT", - "keyID": "2371" - }, - { - "keyString": "Catalogs", - "keySystem": "UAT", - "keyID": "205" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 2023. The Author(s). Published by the American Astronomical Society." - }, - "openAccess": { - "open": true, - "license": "\n\nOriginal content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.", - "licenseURL": "http://creativecommons.org/licenses/by/4.0/" - }, - "funding": [ - { - "agencyname": "MINCyT \u2223 Agencia Nacional de Promoci\u00f3n Cient\u00edfica y Tecnol\u00f3gica (ANPCyT)\n", - "agencyid": { - "idschema": "doi", - "idvalue": "https://doi.org/10.13039/501100003074" - }, - "awardnumber": "0" - } - ] + "title": { + "textEnglish": "A Catalog of the Highest-energy Cosmic Rays Recorded during Phase I of Operation of the Pierre Auger Observatory" + } } diff --git a/tests/stubdata/output/jats_iop_preprint_in_record.json b/tests/stubdata/output/jats_iop_preprint_in_record.json index 384f727..61cf366 100644 --- a/tests/stubdata/output/jats_iop_preprint_in_record.json +++ b/tests/stubdata/output/jats_iop_preprint_in_record.json @@ -1,110 +1,126 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2022-10-11" - ], - "acceptedDate": "2023-04-13" - }, - "pubDate": { - "electrDate": "2023-05-02", - "printDate": "2023-05-01" - }, - "publication": { - "pubName": "Journal of Cosmology and Astroparticle Physics", - "publisher": "IOP Publishing", - "issueNum": "05", - "volumeNum": "2023", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "epub", - "issnString": "1475-7516" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1088/1475-7516/2023/05/001", - "preprint": { - "source": "arxiv", - "identifier": "2210.04800" - } - } - ], - "publisherIDs": [ - { - "attribute": "publisher-id", - "Identifier": "JCAP_029P_1022" - }, - { - "attribute": "manuscript", - "Identifier": "JCAP_029P_1022" - } - ], - "pagination": { - "pageCount": "35", - "electronicID": "001" + "abstract": { + "textEnglish": "Upcoming large-scale structure surveys can shed new light on the properties of dark energy. In particular, if dark energy is a dynamical component, it must have spatial perturbations. Their behaviour is regulated by the speed of sound parameter, which is currently unconstrained. In this work, we present the numerical methods that will allow to perform cosmological simulations of inhomogeneous dark energy scenarios where the speed of sound is small and non-vanishing. We treat the dark energy component as an effective fluid and build upon established numerical methods for hydrodynamics to construct a numerical solution of the effective continuity and Euler equations. In particular, we develop conservative finite volume schemes that rely on the solution of the Riemann problem, which we provide here in both exact and approximate forms for the case of a dark energy fluid." }, "authors": [ { - "name": { - "surname": "Blot", - "given_name": "Linda" - }, "affiliation": [ { - "affPubRaw": "Max Planck Institute for Astrophysics, Karl-Schwarzschild str. 1, 85748 Garching, Germany", - "affPubID": "affiliation01" + "affPubID": "affiliation01", + "affPubRaw": "Max Planck Institute for Astrophysics, Karl-Schwarzschild str. 1, 85748 Garching, Germany" } ], "attrib": { "email": "lblot@mpa-garching.mpg.de" + }, + "name": { + "given_name": "Linda", + "surname": "Blot" } }, { - "name": { - "surname": "Corasaniti", - "given_name": "Pier Stefano" - }, "affiliation": [ { - "affPubRaw": "Laboratoire Univers et Th\u00e9ories (LUTh), UMR 8102 CNRS, Observatoire de Paris, Universit\u00e9 Paris Diderot, 5 Place Jules Janssen, 92190 Meudon, France", - "affPubID": "affiliation02" + "affPubID": "affiliation02", + "affPubRaw": "Laboratoire Univers et Th\u00e9ories (LUTh), UMR 8102 CNRS, Observatoire de Paris, Universit\u00e9 Paris Diderot, 5 Place Jules Janssen, 92190 Meudon, France" } ], "attrib": { "email": "pier-stefano.corasaniti@obspm.fr" + }, + "name": { + "given_name": "Pier Stefano", + "surname": "Corasaniti" } }, { - "name": { - "surname": "Schmidt", - "given_name": "Fabian" - }, "affiliation": [ { - "affPubRaw": "Max Planck Institute for Astrophysics, Karl-Schwarzschild str. 1, 85748 Garching, Germany", - "affPubID": "affiliation01" + "affPubID": "affiliation01", + "affPubRaw": "Max Planck Institute for Astrophysics, Karl-Schwarzschild str. 1, 85748 Garching, Germany" } ], "attrib": { "email": "fabians@mpa-garching.mpg.de" + }, + "name": { + "given_name": "Fabian", + "surname": "Schmidt" } } ], - "title": { - "textEnglish": "Non-linear Eulerian hydrodynamics of dark energy: Riemann problem and finite volume schemes" + "copyright": { + "statement": "\u00a9 2023 The Author(s)", + "status": true }, - "abstract": { - "textEnglish": "Upcoming large-scale structure surveys can shed new light on the properties of dark energy. In particular, if dark energy is a dynamical component, it must have spatial perturbations. Their behaviour is regulated by the speed of sound parameter, which is currently unconstrained. In this work, we present the numerical methods that will allow to perform cosmological simulations of inhomogeneous dark energy scenarios where the speed of sound is small and non-vanishing. We treat the dark energy component as an effective fluid and build upon established numerical methods for hydrodynamics to construct a numerical solution of the effective continuity and Euler equations. In particular, we develop conservative finite volume schemes that rely on the solution of the Riemann problem, which we provide here in both exact and approximate forms for the case of a dark energy fluid." + "editorialHistory": { + "acceptedDate": "2023-04-13", + "receivedDates": [ + "2022-10-11" + ] + }, + "keywords": [ + { + "keyString": "cosmological simulations", + "keySystem": "misc" + }, + { + "keyString": "dark energy theory", + "keySystem": "misc" + } + ], + "openAccess": { + "license": "\nPublished by IOP Publishing Ltd on behalf of Sissa Medialab. Original content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.", + "licenseURL": "http://creativecommons.org/licenses/by/4.0", + "open": true + }, + "pagination": { + "electronicID": "001", + "pageCount": "35" + }, + "persistentIDs": [ + { + "DOI": "10.1088/1475-7516/2023/05/001", + "preprint": { + "identifier": "2210.04800", + "source": "arxiv" + } + } + ], + "pubDate": { + "electrDate": "2023-05-02", + "printDate": "2023-05-01" + }, + "publication": { + "ISSN": [ + { + "issnString": "1475-7516", + "pubtype": "epub" + } + ], + "issueNum": "05", + "pubName": "Journal of Cosmology and Astroparticle Physics", + "pubYear": "2023", + "publisher": "IOP Publishing", + "volumeNum": "2023" + }, + "publisherIDs": [ + { + "Identifier": "JCAP_029P_1022", + "attribute": "publisher-id" + }, + { + "Identifier": "JCAP_029P_1022", + "attribute": "manuscript" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " Planck Collaboration AghanimN. Planck 2018 results. VI. Cosmological parametersAstron. Astrophys.2020641A610.1051/0004-6361/201833910(arXiv:1807.06209)[Erratum: Astron.Astrophys. 652, C4 (2021)]", @@ -163,23 +179,7 @@ " M. Zingale, Introduction to Computational Astrophysical Hydrodynamics, http://bender.astro.sunysb.edu/hydro_by_example/CompHydroTutorial.pdf. ", " ColellaPhillip WoodwardPaul R. The Piecewise Parabolic Method (PPM) for Gas Dynamical SimulationsJ. Comput. Phys.19845417420110.1016/0021-9991(84)90143-8" ], - "keywords": [ - { - "keyString": "cosmological simulations", - "keySystem": "misc" - }, - { - "keyString": "dark energy theory", - "keySystem": "misc" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 2023 The Author(s)" - }, - "openAccess": { - "open": true, - "license": "\nPublished by IOP Publishing Ltd on behalf of Sissa Medialab. Original content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.", - "licenseURL": "http://creativecommons.org/licenses/by/4.0" + "title": { + "textEnglish": "Non-linear Eulerian hydrodynamics of dark energy: Riemann problem and finite volume schemes" } } diff --git a/tests/stubdata/output/jats_mnras_493_1_141.json b/tests/stubdata/output/jats_mnras_493_1_141.json index d8de9f8..602c005 100644 --- a/tests/stubdata/output/jats_mnras_493_1_141.json +++ b/tests/stubdata/output/jats_mnras_493_1_141.json @@ -1,201 +1,239 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2019-10-07" - ], - "revisedDates": [ - "2019-12-14" - ], - "acceptedDate": "2020-01-06" - }, - "pubDate": { - "electrDate": "2020-01-14", - "printDate": "2020-03-00" - }, - "publication": { - "pubName": "Monthly Notices of the Royal Astronomical Society", - "publisher": "Oxford University Press", - "issueNum": "1", - "volumeNum": "493", - "pubYear": "2020", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "0035-8711" - }, - { - "pubtype": "epub", - "issnString": "1365-2966" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1093/mnras/staa093" - } - ], - "publisherIDs": [ - { - "attribute": "publisher-id", - "Identifier": "staa093" - } - ], - "pagination": { - "firstPage": "141", - "lastPage": "160", - "pageCount": "20", - "pageRange": "141-160" + "abstract": { + "textEnglish": "We explore deep rest-frame UV to FIR data in the COSMOS field to measure the individual spectral energy distributions (SED) of the \u223c4000 SC4K (Sobral et al.) Lyman \u03b1 (Ly \u03b1) emitters (LAEs) at z \u223c 2\u20136. We find typical stellar masses of 109.3 \u00b1 0.6 M\u2299 and star formation rates (SFR) of SFR$_{\\rm SED}=4.4^{+10.5}_{-2.4}$ M\u2299 yr\u22121 and SFR$_{\\rm Ly\\,\\alpha }=5.9^{+6.3}_{-2.6}$ M\u2299 yr\u22121, combined with very blue UV slopes of $\\beta =-2.1^{+0.5}_{-0.4}$, but with significant variations within the population. MUV and \u03b2 are correlated in a similar way to UV-selected sources, but LAEs are consistently bluer. This suggests that LAEs are the youngest and/or most dust-poor subset of the UV-selected population. We also study the Ly \u03b1 rest-frame equivalent width (EW0) and find 45 \u2018extreme\u2019 LAEs with EW0 > 240 \u00c5 (3\u03c3), implying a low number density of (7 \u00b1 1) \u00d7 10\u22127 Mpc\u22123. Overall, we measure little to no evolution of the Ly \u03b1 EW0 and scale length parameter (w0), which are consistently high (EW$_0=140^{+280}_{-70}$ \u00c5, $w_0=129^{+11}_{-11}$ \u00c5) from z \u223c 6 to z \u223c 2 and below. However, w0 is anticorrelated with MUV and stellar mass. Our results imply that sources selected as LAEs have a high Ly \u03b1 escape fraction (fesc,Ly \u03b1) irrespective of cosmic time, but fesc,Ly \u03b1 is still higher for UV-fainter and lower mass LAEs. The least massive LAEs (<109.5 M\u2299) are typically located above the star formation \u2018main sequence\u2019 (MS), but the offset from the MS decreases towards z \u223c 6 and towards 1010 M\u2299. Our results imply a lack of evolution in the properties of LAEs across time and reveals the increasing overlap in properties of LAEs and UV-continuum selected galaxies as typical star-forming galaxies at high redshift effectively become LAEs." }, "authors": [ { - "name": { - "surname": "Santos", - "given_name": "S" - }, "affiliation": [ { - "affPubRaw": "Department of Physics, Lancaster University, Lancaster LA1 4YB, UK", - "affPubID": "aff1" + "affPubID": "aff1", + "affPubRaw": "Department of Physics, Lancaster University, Lancaster LA1 4YB, UK" } ], "attrib": { "email": "s.santos@lancaster.ac.uk" + }, + "name": { + "given_name": "S", + "surname": "Santos" } }, { - "name": { - "surname": "Sobral", - "given_name": "D" - }, "affiliation": [ { - "affPubRaw": "Department of Physics, Lancaster University, Lancaster LA1 4YB, UK", - "affPubID": "aff1" + "affPubID": "aff1", + "affPubRaw": "Department of Physics, Lancaster University, Lancaster LA1 4YB, UK" } ], "attrib": { "orcid": "0000-0001-8823-4845" + }, + "name": { + "given_name": "D", + "surname": "Sobral" } }, { - "name": { - "surname": "Matthee", - "given_name": "J" - }, "affiliation": [ { - "affPubRaw": "Department of Physics, ETH Z\u00fcrich, Wolfgang-Pauli-Strasse 27, CH-8093 Z\u00fcrich, Switzerland", - "affPubID": "aff2" + "affPubID": "aff2", + "affPubRaw": "Department of Physics, ETH Z\u00fcrich, Wolfgang-Pauli-Strasse 27, CH-8093 Z\u00fcrich, Switzerland" } ], "attrib": { "orcid": "0000-0003-2871-127X" + }, + "name": { + "given_name": "J", + "surname": "Matthee" } }, { - "name": { - "surname": "Calhau", - "given_name": "J" - }, "affiliation": [ { - "affPubRaw": "Department of Physics, Lancaster University, Lancaster LA1 4YB, UK", - "affPubID": "aff1" + "affPubID": "aff1", + "affPubRaw": "Department of Physics, Lancaster University, Lancaster LA1 4YB, UK" } - ] + ], + "name": { + "given_name": "J", + "surname": "Calhau" + } }, { - "name": { - "surname": "da Cunha", - "given_name": "E" - }, "affiliation": [ { - "affPubRaw": "International Centre for Radio Astronomy Research, University of Western Australia, 35 Stirling Hwy, Crawley, WA 6009, Australia", - "affPubID": "aff3" + "affPubID": "aff3", + "affPubRaw": "International Centre for Radio Astronomy Research, University of Western Australia, 35 Stirling Hwy, Crawley, WA 6009, Australia" }, { - "affPubRaw": "Research School of Astronomy and Astrophysics, The Australian National University, Canberra, ACT 2611, Australia", - "affPubID": "aff4" + "affPubID": "aff4", + "affPubRaw": "Research School of Astronomy and Astrophysics, The Australian National University, Canberra, ACT 2611, Australia" }, { - "affPubRaw": "ARC Centre of Excellence for All Sky Astrophysics in 3 Dimensions (ASTRO 3D), Millers Point NSW 2000, Australia", - "affPubID": "aff5" + "affPubID": "aff5", + "affPubRaw": "ARC Centre of Excellence for All Sky Astrophysics in 3 Dimensions (ASTRO 3D), Millers Point NSW 2000, Australia" } - ] + ], + "name": { + "given_name": "E", + "surname": "da Cunha" + } }, { - "name": { - "surname": "Ribeiro", - "given_name": "B" - }, "affiliation": [ { - "affPubRaw": "Leiden Observatory, Leiden University, PO Box 9513, NL-2300 RA Leiden, the Netherlands", - "affPubID": "aff6" + "affPubID": "aff6", + "affPubRaw": "Leiden Observatory, Leiden University, PO Box 9513, NL-2300 RA Leiden, the Netherlands" } - ] + ], + "name": { + "given_name": "B", + "surname": "Ribeiro" + } }, { - "name": { - "surname": "Paulino-Afonso", - "given_name": "A" - }, "affiliation": [ { - "affPubRaw": "CENTRA - Centro de Astrof\u00edsica e Gravita\u00e7\u00e3o, Instituto Superior T\u00e9cnico, Av. Rovisco Pais, 1, P-1049-001 Lisboa, Portugal", - "affPubID": "aff7" + "affPubID": "aff7", + "affPubRaw": "CENTRA - Centro de Astrof\u00edsica e Gravita\u00e7\u00e3o, Instituto Superior T\u00e9cnico, Av. Rovisco Pais, 1, P-1049-001 Lisboa, Portugal" } ], "attrib": { "orcid": "0000-0002-0943-0694" + }, + "name": { + "given_name": "A", + "surname": "Paulino-Afonso" } }, { - "name": { - "surname": "Arrabal Haro", - "given_name": "P" - }, "affiliation": [ { - "affPubRaw": "Instituto de Astrof\u00edsica de Canarias (IAC), E-38205 La Laguna, Spain", - "affPubID": "aff8" + "affPubID": "aff8", + "affPubRaw": "Instituto de Astrof\u00edsica de Canarias (IAC), E-38205 La Laguna, Spain" }, { - "affPubRaw": "Departamento de Astrof\u00edsica, Universidad de La Laguna, E-38206 La Laguna, Spain", - "affPubID": "aff9" + "affPubID": "aff9", + "affPubRaw": "Departamento de Astrof\u00edsica, Universidad de La Laguna, E-38206 La Laguna, Spain" } ], "attrib": { "orcid": "0000-0002-7959-8783" + }, + "name": { + "given_name": "P", + "surname": "Arrabal Haro" } }, { - "name": { - "surname": "Butterworth", - "given_name": "J" - }, "affiliation": [ { - "affPubRaw": "Department of Physics, Lancaster University, Lancaster LA1 4YB, UK", - "affPubID": "aff1" + "affPubID": "aff1", + "affPubRaw": "Department of Physics, Lancaster University, Lancaster LA1 4YB, UK" } - ] + ], + "name": { + "given_name": "J", + "surname": "Butterworth" + } } ], - "title": { - "textEnglish": "The evolution of rest-frame UV properties, Ly \u03b1 EWs, and the SFR\u2013stellar mass relation at z \u223c 2\u20136 for SC4K LAEs" + "copyright": { + "statement": "\u00a9 2020 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society", + "status": true }, - "abstract": { - "textEnglish": "We explore deep rest-frame UV to FIR data in the COSMOS field to measure the individual spectral energy distributions (SED) of the \u223c4000 SC4K (Sobral et al.) Lyman \u03b1 (Ly \u03b1) emitters (LAEs) at z \u223c 2\u20136. We find typical stellar masses of 109.3 \u00b1 0.6 M\u2299 and star formation rates (SFR) of SFR$_{\\rm SED}=4.4^{+10.5}_{-2.4}$ M\u2299 yr\u22121 and SFR$_{\\rm Ly\\,\\alpha }=5.9^{+6.3}_{-2.6}$ M\u2299 yr\u22121, combined with very blue UV slopes of $\\beta =-2.1^{+0.5}_{-0.4}$, but with significant variations within the population. MUV and \u03b2 are correlated in a similar way to UV-selected sources, but LAEs are consistently bluer. This suggests that LAEs are the youngest and/or most dust-poor subset of the UV-selected population. We also study the Ly \u03b1 rest-frame equivalent width (EW0) and find 45 \u2018extreme\u2019 LAEs with EW0 > 240 \u00c5 (3\u03c3), implying a low number density of (7 \u00b1 1) \u00d7 10\u22127 Mpc\u22123. Overall, we measure little to no evolution of the Ly \u03b1 EW0 and scale length parameter (w0), which are consistently high (EW$_0=140^{+280}_{-70}$ \u00c5, $w_0=129^{+11}_{-11}$ \u00c5) from z \u223c 6 to z \u223c 2 and below. However, w0 is anticorrelated with MUV and stellar mass. Our results imply that sources selected as LAEs have a high Ly \u03b1 escape fraction (fesc,Ly \u03b1) irrespective of cosmic time, but fesc,Ly \u03b1 is still higher for UV-fainter and lower mass LAEs. The least massive LAEs (<109.5 M\u2299) are typically located above the star formation \u2018main sequence\u2019 (MS), but the offset from the MS decreases towards z \u223c 6 and towards 1010 M\u2299. Our results imply a lack of evolution in the properties of LAEs across time and reveals the increasing overlap in properties of LAEs and UV-continuum selected galaxies as typical star-forming galaxies at high redshift effectively become LAEs." + "editorialHistory": { + "acceptedDate": "2020-01-06", + "receivedDates": [ + "2019-10-07" + ], + "revisedDates": [ + "2019-12-14" + ] + }, + "funding": [ + { + "agencyid": { + "idvalue": "Lancaster University" + }, + "agencyname": "\n\n10.13039/100010029\n\n" + }, + { + "agencyid": { + "idvalue": "Funda\u00e7\u00e3o para a Ci\u00eancia e a Tecnologia" + }, + "agencyname": "\n\n10.13039/501100001871\n\n", + "awardnumber": "PTDC/FIS-AST/31546/2017" + } + ], + "keywords": [ + { + "keyString": "galaxies: evolution", + "keySystem": "misc" + }, + { + "keyString": "galaxies: formation", + "keySystem": "misc" + }, + { + "keyString": "galaxies: high-redshift", + "keySystem": "misc" + }, + { + "keyString": "galaxies: star formation", + "keySystem": "misc" + } + ], + "openAccess": { + "license": "This article is published and distributed under the terms of the Oxford University Press, Standard Journals Publication Model (https://academic.oup.com/journals/pages/open_access/funder_policies/chorus/standard_publication_model)", + "licenseURL": "https://academic.oup.com/journals/pages/open_access/funder_policies/chorus/standard_publication_model" + }, + "pagination": { + "firstPage": "141", + "lastPage": "160", + "pageCount": "20", + "pageRange": "141-160" + }, + "persistentIDs": [ + { + "DOI": "10.1093/mnras/staa093" + } + ], + "pubDate": { + "electrDate": "2020-01-14", + "printDate": "2020-03-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "0035-8711", + "pubtype": "ppub" + }, + { + "issnString": "1365-2966", + "pubtype": "epub" + } + ], + "issueNum": "1", + "pubName": "Monthly Notices of the Royal Astronomical Society", + "pubYear": "2020", + "publisher": "Oxford University Press", + "volumeNum": "493" + }, + "publisherIDs": [ + { + "Identifier": "staa093", + "attribute": "publisher-id" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " Adams J. J. et al., 2011, ApJS, 192, 510.1088/0067-0049/192/1/5 ", @@ -332,45 +370,7 @@ " Wold I. G. B. , FinkelsteinS. L., BargerA. J., CowieL. L., RosenwasserB., 2017, ApJ, 848, 10810.3847/1538-4357/aa8d6b ", " Yajima H. , LiY., ZhuQ., AbelT., GronwallC., CiardulloR., 2012, ApJ, 754, 11810.1088/0004-637X/754/2/118 " ], - "keywords": [ - { - "keyString": "galaxies: evolution", - "keySystem": "misc" - }, - { - "keyString": "galaxies: formation", - "keySystem": "misc" - }, - { - "keyString": "galaxies: high-redshift", - "keySystem": "misc" - }, - { - "keyString": "galaxies: star formation", - "keySystem": "misc" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 2020 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society" - }, - "openAccess": { - "license": "This article is published and distributed under the terms of the Oxford University Press, Standard Journals Publication Model (https://academic.oup.com/journals/pages/open_access/funder_policies/chorus/standard_publication_model)", - "licenseURL": "https://academic.oup.com/journals/pages/open_access/funder_policies/chorus/standard_publication_model" - }, - "funding": [ - { - "agencyname": "\n\n10.13039/100010029\n\n", - "agencyid": { - "idvalue": "Lancaster University" - } - }, - { - "agencyname": "\n\n10.13039/501100001871\n\n", - "agencyid": { - "idvalue": "Funda\u00e7\u00e3o para a Ci\u00eancia e a Tecnologia" - }, - "awardnumber": "PTDC/FIS-AST/31546/2017" - } - ] + "title": { + "textEnglish": "The evolution of rest-frame UV properties, Ly \u03b1 EWs, and the SFR\u2013stellar mass relation at z \u223c 2\u20136 for SC4K LAEs" + } } diff --git a/tests/stubdata/output/jats_phrvd_106_023001.json b/tests/stubdata/output/jats_phrvd_106_023001.json index 0722163..eb69d6b 100644 --- a/tests/stubdata/output/jats_phrvd_106_023001.json +++ b/tests/stubdata/output/jats_phrvd_106_023001.json @@ -1,98 +1,172 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2022-07-01", - "printDate": "2022-07-15" - }, - "publication": { - "pubName": "Physical Review D", - "publisher": "American Physical Society", - "issueNum": "2", - "volumeNum": "106", - "pubYear": "2022", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "2470-0010" - }, - { - "pubtype": "epub", - "issnString": "2470-0029" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1103/PhysRevD.106.023001" - } - ], - "pagination": { - "pageCount": "28", - "electronicID": "023001" + "abstract": { + "textEnglish": "Two important parameters inferred from the gravitational wave signals of binaries of precessing black holes are the spin tilt angles, i.e., the angles at which the black holes\u2019 spin axes are inclined with respect to the binary\u2019s orbital angular momentum. The LIGO-Virgo parameter estimation analyses provide spin tilts at a fiducial reference frequency, often the lowest frequency used in the data analysis. However, the most astrophysically interesting quantities are the spin tilts when the binary was formed, which can be significantly different from those at the reference frequency for strongly precessing binaries. The spin tilts at formally infinite separation are a good approximation to the tilts at formation in many formation channels and can be computed efficiently for binary black holes using precession-averaged evolution. Here, we present a new code for computing the tilts at infinity that combines the precession-averaged evolution with orbit-averaged evolution at high frequencies and illustrate its application to GW190521 and other binary black hole detections from O3. We have empirically determined the transition frequency between the orbit-averaged and precession-averaged evolution to produce tilts at infinity with a given accuracy and find that using only the precession-averaged evolution can lead to errors in the cosines of the tilts at infinity of > 0.8 for certain binary configurations. However, the precession-averaged evolution alone is sufficient for good accuracy when obtaining the posterior distributions of the tilts at infinity for current detections. We also have regularized the precession-averaged equations in order to obtain good accuracy for the very close-to-equal-mass binary parameters encountered in practice. This additionally allows us to investigate the singular equal-mass limit of the precession-averaged expressions, where we find that to a good approximation the results only depend on the orbital angular momentum L through the combination ( 1 - q ) L , where q is the mass ratio." }, "authors": [ { - "name": { - "surname": "Johnson-McDaniel", - "given_name": "Nathan K." - }, "affiliation": [ { - "affPubRaw": "Department of Applied Mathematics and Theoretical Physics, Centre for Mathematical Sciences, University of Cambridge, Wilberforce Road, Cambridge CB3 0WA, United Kingdom", - "affPubID": "a1" + "affPubID": "a1", + "affPubRaw": "Department of Applied Mathematics and Theoretical Physics, Centre for Mathematical Sciences, University of Cambridge, Wilberforce Road, Cambridge CB3 0WA, United Kingdom" }, { - "affPubRaw": "Department of Physics and Astronomy, The University of Mississippi, University, Mississippi 38677, USA", - "affPubID": "a2" + "affPubID": "a2", + "affPubRaw": "Department of Physics and Astronomy, The University of Mississippi, University, Mississippi 38677, USA" } ], "attrib": { "orcid": "0000-0001-5357-9480" + }, + "name": { + "given_name": "Nathan K.", + "surname": "Johnson-McDaniel" } }, { - "name": { - "surname": "Kulkarni", - "given_name": "Sumeet" - }, "affiliation": [ { - "affPubRaw": "Department of Physics and Astronomy, The University of Mississippi, University, Mississippi 38677, USA", - "affPubID": "a2" + "affPubID": "a2", + "affPubRaw": "Department of Physics and Astronomy, The University of Mississippi, University, Mississippi 38677, USA" } ], "attrib": { "orcid": "0000-0001-8057-0203" + }, + "name": { + "given_name": "Sumeet", + "surname": "Kulkarni" } }, { - "name": { - "surname": "Gupta", - "given_name": "Anuradha" - }, "affiliation": [ { - "affPubRaw": "Department of Physics and Astronomy, The University of Mississippi, University, Mississippi 38677, USA", - "affPubID": "a2" + "affPubID": "a2", + "affPubRaw": "Department of Physics and Astronomy, The University of Mississippi, University, Mississippi 38677, USA" } ], "attrib": { "orcid": "0000-0002-5441-9013" + }, + "name": { + "given_name": "Anuradha", + "surname": "Gupta" } } ], - "title": { - "textEnglish": "Inferring spin tilts at formation from gravitational wave observations of binary black holes: Interfacing precession-averaged and orbit-averaged spin evolution" + "copyright": { + "statement": "\u00a9 2022 American Physical Society", + "status": true }, - "abstract": { - "textEnglish": "Two important parameters inferred from the gravitational wave signals of binaries of precessing black holes are the spin tilt angles, i.e., the angles at which the black holes\u2019 spin axes are inclined with respect to the binary\u2019s orbital angular momentum. The LIGO-Virgo parameter estimation analyses provide spin tilts at a fiducial reference frequency, often the lowest frequency used in the data analysis. However, the most astrophysically interesting quantities are the spin tilts when the binary was formed, which can be significantly different from those at the reference frequency for strongly precessing binaries. The spin tilts at formally infinite separation are a good approximation to the tilts at formation in many formation channels and can be computed efficiently for binary black holes using precession-averaged evolution. Here, we present a new code for computing the tilts at infinity that combines the precession-averaged evolution with orbit-averaged evolution at high frequencies and illustrate its application to GW190521 and other binary black hole detections from O3. We have empirically determined the transition frequency between the orbit-averaged and precession-averaged evolution to produce tilts at infinity with a given accuracy and find that using only the precession-averaged evolution can lead to errors in the cosines of the tilts at infinity of > 0.8 for certain binary configurations. However, the precession-averaged evolution alone is sufficient for good accuracy when obtaining the posterior distributions of the tilts at infinity for current detections. We also have regularized the precession-averaged equations in order to obtain good accuracy for the very close-to-equal-mass binary parameters encountered in practice. This additionally allows us to investigate the singular equal-mass limit of the precession-averaged expressions, where we find that to a good approximation the results only depend on the orbital angular momentum L through the combination ( 1 - q ) L , where q is the mass ratio." + "funding": [ + { + "agencyid": { + "idschema": "doi", + "idvalue": "10.13039/501100000271" + }, + "agencyname": "Science and Technology Facilities Council", + "awardnumber": "ST/L000636/1" + }, + { + "agencyid": { + "idschema": "doi", + "idvalue": "10.13039/100010661" + }, + "agencyname": "Horizon 2020 Framework Programme" + }, + { + "agencyid": { + "idschema": "doi", + "idvalue": "10.13039/100010665" + }, + "agencyname": "H2020 Marie Sk\u0142odowska-Curie Actions", + "awardnumber": "690904" + }, + { + "agencyid": { + "idschema": "doi", + "idvalue": "10.13039/501100021745" + }, + "agencyname": "Institut P\u00e9rim\u00e8tre de physique th\u00e9orique" + }, + { + "agencyid": { + "idschema": "doi", + "idvalue": "10.13039/501100000023" + }, + "agencyname": "Government of Canada" + }, + { + "agencyid": { + "idschema": "doi", + "idvalue": "10.13039/501100000192" + }, + "agencyname": "Ontario Ministry of Economic Development and Innovation" + }, + { + "agencyid": { + "idschema": "doi", + "idvalue": "10.13039/501100003204" + }, + "agencyname": "Airbus" + }, + { + "agencyid": { + "idschema": "doi", + "idvalue": "10.13039/100017167" + }, + "agencyname": "International Centre for Theoretical Sciences" + }, + { + "agencyid": { + "idschema": "doi", + "idvalue": "10.13039/501100001405" + }, + "agencyname": "Tata Institute of Fundamental Research" + } + ], + "keywords": [ + { + "keyString": "Astrophysics and astroparticle physics", + "keySystem": "subject" + } + ], + "pagination": { + "electronicID": "023001", + "pageCount": "28" + }, + "persistentIDs": [ + { + "DOI": "10.1103/PhysRevD.106.023001" + } + ], + "pubDate": { + "electrDate": "2022-07-01", + "printDate": "2022-07-15" + }, + "publication": { + "ISSN": [ + { + "issnString": "2470-0010", + "pubtype": "ppub" + }, + { + "issnString": "2470-0029", + "pubtype": "epub" + } + ], + "issueNum": "2", + "pubName": "Physical Review D", + "pubYear": "2022", + "publisher": "American Physical Society", + "volumeNum": "106" + }, + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " 1 R. Abbott ( \t\t\t\t\t\tLIGO Scientific Collaboration and Virgo Collaboration) \t\t\t\t\t, \t\t\t\t\tPhys. Rev. D 102, \t\t\t\t\t043015 ( \t\t\t\t\t2020). \t\t\t\t\tPRVDAQ 2470-0010 10.1103/PhysRevD.102.043015 ", @@ -187,81 +261,7 @@ " 90 J.\u2009D. Hunter , \t\t\t\t\tComput. Sci. Eng. 9, \t\t\t\t\t90 ( \t\t\t\t\t2007). \t\t\t\t\tCSENFA 1521-9615 10.1109/MCSE.2007.55 ", " 91 M. Abramowitz and \t\t\t\t\t\tI.\u2009A. Stegun, eds. \t\t\t\t\t, \t\t\t\t\tHandbook of Mathematical Functions With Formulas, Graphs, and Mathematical Tables, \t\t\t\t\tApplied Mathematics Series No. 55 ( \t\t\t\t\tNational Bureau of Standards, Washington, D.C., \t\t\t\t\t1964). \t\t\t\t " ], - "keywords": [ - { - "keyString": "Astrophysics and astroparticle physics", - "keySystem": "subject" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 2022 American Physical Society" - }, - "funding": [ - { - "agencyname": "Science and Technology Facilities Council", - "agencyid": { - "idschema": "doi", - "idvalue": "10.13039/501100000271" - }, - "awardnumber": "ST/L000636/1" - }, - { - "agencyname": "Horizon 2020 Framework Programme", - "agencyid": { - "idschema": "doi", - "idvalue": "10.13039/100010661" - } - }, - { - "agencyname": "H2020 Marie Sk\u0142odowska-Curie Actions", - "agencyid": { - "idschema": "doi", - "idvalue": "10.13039/100010665" - }, - "awardnumber": "690904" - }, - { - "agencyname": "Institut P\u00e9rim\u00e8tre de physique th\u00e9orique", - "agencyid": { - "idschema": "doi", - "idvalue": "10.13039/501100021745" - } - }, - { - "agencyname": "Government of Canada", - "agencyid": { - "idschema": "doi", - "idvalue": "10.13039/501100000023" - } - }, - { - "agencyname": "Ontario Ministry of Economic Development and Innovation", - "agencyid": { - "idschema": "doi", - "idvalue": "10.13039/501100000192" - } - }, - { - "agencyname": "Airbus", - "agencyid": { - "idschema": "doi", - "idvalue": "10.13039/501100003204" - } - }, - { - "agencyname": "International Centre for Theoretical Sciences", - "agencyid": { - "idschema": "doi", - "idvalue": "10.13039/100017167" - } - }, - { - "agencyname": "Tata Institute of Fundamental Research", - "agencyid": { - "idschema": "doi", - "idvalue": "10.13039/501100001405" - } - } - ] + "title": { + "textEnglish": "Inferring spin tilts at formation from gravitational wave observations of binary black holes: Interfacing precession-averaged and orbit-averaged spin evolution" + } } diff --git a/tests/stubdata/output/jats_pnas_1715554115.json b/tests/stubdata/output/jats_pnas_1715554115.json index 5380b57..61253d8 100644 --- a/tests/stubdata/output/jats_pnas_1715554115.json +++ b/tests/stubdata/output/jats_pnas_1715554115.json @@ -1,224 +1,181 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2018-02-05", - "printDate": "2018-02-20" - }, - "publication": { - "pubName": "Proceedings of the National Academy of Sciences", - "publisher": "National Academy of Sciences", - "issueNum": "8", - "volumeNum": "115", - "pubYear": "2018", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "0027-8424" - }, - { - "pubtype": "epub", - "issnString": "1091-6490" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1073/pnas.1715554115" - } - ], - "publisherIDs": [ - { - "attribute": "publisher-id", - "Identifier": "201715554" - } - ], - "pagination": { - "firstPage": "1697", - "lastPage": "1706", - "pageCount": "10", - "pageRange": "1697-1706" + "abstract": { + "textEnglish": "Alzheimer\u2019s disease (AD) is an age-related neurodegenerative disease. Genome-wide association studies predominately focusing on Caucasian populations have identified risk loci and genes associated with AD; the majority of these variants reside in noncoding regions with unclear functions. Here, we report a whole-genome sequencing study for AD in the Chinese population. Other than the APOE locus, we identified common variants in GCH1 and KCNJ15 that show suggestive associations with AD. For these two risk variants, an association with AD or advanced onset of disease can be observed in non-Asian AD cohorts. An association study of risk variants with expression data revealed their modulatory effects on immune signatures, linking the potential roles of these genes with immune-related pathways during AD pathogenesis." }, "authors": [ { - "name": { - "surname": "Zhou", - "given_name": "Xiaopu" - }, "affiliation": [ { - "affPubRaw": "Division of Life Science, State Key Laboratory of Molecular Neuroscience and Molecular Neuroscience Center, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China", - "affPubID": "aff1" + "affPubID": "aff1", + "affPubRaw": "Division of Life Science, State Key Laboratory of Molecular Neuroscience and Molecular Neuroscience Center, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China" } - ] + ], + "name": { + "given_name": "Xiaopu", + "surname": "Zhou" + } }, { - "name": { - "surname": "Chen", - "given_name": "Yu" - }, "affiliation": [ { - "affPubRaw": "Division of Life Science, State Key Laboratory of Molecular Neuroscience and Molecular Neuroscience Center, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China", - "affPubID": "aff1" + "affPubID": "aff1", + "affPubRaw": "Division of Life Science, State Key Laboratory of Molecular Neuroscience and Molecular Neuroscience Center, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China" }, { - "affPubRaw": "Guangdong Provincial Key Laboratory of Brain Science, Disease, and Drug Development, Hong Kong University of Science and Technology Shenzhen Research Institute, Shenzhen, 518057 Guangdong, China", - "affPubID": "aff2" + "affPubID": "aff2", + "affPubRaw": "Guangdong Provincial Key Laboratory of Brain Science, Disease, and Drug Development, Hong Kong University of Science and Technology Shenzhen Research Institute, Shenzhen, 518057 Guangdong, China" }, { - "affPubRaw": "The Brain Cognition and Brain Disease Institute, Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen, 518055 Guangdong, China", - "affPubID": "aff3" + "affPubID": "aff3", + "affPubRaw": "The Brain Cognition and Brain Disease Institute, Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen, 518055 Guangdong, China" } - ] + ], + "name": { + "given_name": "Yu", + "surname": "Chen" + } }, { - "name": { - "surname": "Mok", - "given_name": "Kin Y." - }, "affiliation": [ { - "affPubRaw": "Division of Life Science, State Key Laboratory of Molecular Neuroscience and Molecular Neuroscience Center, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China", - "affPubID": "aff1" + "affPubID": "aff1", + "affPubRaw": "Division of Life Science, State Key Laboratory of Molecular Neuroscience and Molecular Neuroscience Center, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China" }, { - "affPubRaw": "Department of Molecular Neuroscience, University College London Institute of Neurology, London WC1N 3BG, United Kingdom", - "affPubID": "aff4" + "affPubID": "aff4", + "affPubRaw": "Department of Molecular Neuroscience, University College London Institute of Neurology, London WC1N 3BG, United Kingdom" } - ] + ], + "name": { + "given_name": "Kin Y.", + "surname": "Mok" + } }, { - "name": { - "surname": "Zhao", - "given_name": "Qianhua" - }, "affiliation": [ { - "affPubRaw": "Department of Neurology, Huashan Hospital, Fudan University, 200040 Shanghai, China", - "affPubID": "aff5" + "affPubID": "aff5", + "affPubRaw": "Department of Neurology, Huashan Hospital, Fudan University, 200040 Shanghai, China" } - ] + ], + "name": { + "given_name": "Qianhua", + "surname": "Zhao" + } }, { - "name": { - "surname": "Chen", - "given_name": "Keliang" - }, "affiliation": [ { - "affPubRaw": "Department of Neurology, Huashan Hospital, Fudan University, 200040 Shanghai, China", - "affPubID": "aff5" + "affPubID": "aff5", + "affPubRaw": "Department of Neurology, Huashan Hospital, Fudan University, 200040 Shanghai, China" } - ] + ], + "name": { + "given_name": "Keliang", + "surname": "Chen" + } }, { - "name": { - "surname": "Chen", - "given_name": "Yuewen" - }, "affiliation": [ { - "affPubRaw": "Division of Life Science, State Key Laboratory of Molecular Neuroscience and Molecular Neuroscience Center, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China", - 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] + ], + "name": { + "given_name": "Yuewen", + "surname": "Chen" + } }, { - "name": { - "surname": "Hardy", - "given_name": "John" - }, "affiliation": [ { - "affPubRaw": "Department of Molecular Neuroscience, University College London Institute of Neurology, London WC1N 3BG, United Kingdom", - "affPubID": "aff4" + "affPubID": "aff4", + "affPubRaw": "Department of Molecular Neuroscience, University College London Institute of Neurology, London WC1N 3BG, United Kingdom" } - ] + ], + "name": { + "given_name": "John", + "surname": "Hardy" + } }, { - "name": { - "surname": "Li", - "given_name": "Yun" - }, "affiliation": [ { - "affPubRaw": "Department of Genetics, University of North Carolina, Chapel Hill, NC 27599", - "affPubID": "aff6" + "affPubID": "aff6", + "affPubRaw": "Department of Genetics, University of North Carolina, Chapel Hill, NC 27599" }, { - "affPubRaw": "Department of Biostatistics, University of North Carolina, Chapel Hill, NC 27599", - "affPubID": "aff7" + "affPubID": "aff7", + "affPubRaw": "Department of Biostatistics, University of North Carolina, Chapel Hill, NC 27599" }, { - "affPubRaw": "Department of Computer Science, University of North Carolina, Chapel Hill, NC 27599", - "affPubID": "aff8" + "affPubID": "aff8", + "affPubRaw": "Department of Computer Science, University of North Carolina, Chapel Hill, NC 27599" } - ] + ], + "name": { + "given_name": "Yun", + "surname": "Li" + } }, { - "name": { - "surname": "Fu", - "given_name": "Amy K. Y." - }, "affiliation": [ { - "affPubRaw": "Division of Life Science, State Key Laboratory of Molecular Neuroscience and Molecular Neuroscience Center, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China", - "affPubID": "aff1" + "affPubID": "aff1", + "affPubRaw": "Division of Life Science, State Key Laboratory of Molecular Neuroscience and Molecular Neuroscience Center, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China" }, { - "affPubRaw": "Guangdong Provincial Key Laboratory of Brain Science, Disease, and Drug Development, Hong Kong University of Science and Technology Shenzhen Research Institute, Shenzhen, 518057 Guangdong, China", - "affPubID": "aff2" + "affPubID": "aff2", + "affPubRaw": "Guangdong Provincial Key Laboratory of Brain Science, Disease, and Drug Development, Hong Kong University of Science and Technology Shenzhen Research Institute, Shenzhen, 518057 Guangdong, China" } - ] + ], + "name": { + "given_name": "Amy K. Y.", + "surname": "Fu" + } }, { - "name": { - "surname": "Guo", - "given_name": "Qihao" - }, "affiliation": [ { - "affPubRaw": "Department of Neurology, Huashan Hospital, Fudan University, 200040 Shanghai, China", - "affPubID": "aff5" + "affPubID": "aff5", + "affPubRaw": "Department of Neurology, Huashan Hospital, Fudan University, 200040 Shanghai, China" } ], "attrib": { "email": "dr.guoqihao@126.com" + }, + "name": { + "given_name": "Qihao", + "surname": "Guo" } }, { - "name": { - "surname": "Ip", - "given_name": "Nancy Y." - }, "affiliation": [ { - "affPubRaw": "Division of Life Science, State Key Laboratory of Molecular Neuroscience and Molecular Neuroscience Center, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China", - "affPubID": "aff1" + "affPubID": "aff1", + "affPubRaw": "Division of Life Science, State Key Laboratory of Molecular Neuroscience and Molecular Neuroscience Center, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China" }, { - "affPubRaw": "Guangdong Provincial Key Laboratory of Brain Science, Disease, and Drug Development, Hong Kong University of Science and Technology Shenzhen Research Institute, Shenzhen, 518057 Guangdong, China", - "affPubID": "aff2" + "affPubID": "aff2", + "affPubRaw": "Guangdong Provincial Key Laboratory of Brain Science, Disease, and Drug Development, Hong Kong University of Science and Technology Shenzhen Research Institute, Shenzhen, 518057 Guangdong, China" } ], "attrib": { "email": "dr.guoqihao@126.com", "orcid": "0000-0002-2763-8907" + }, + "name": { + "given_name": "Nancy Y.", + "surname": "Ip" } }, { @@ -227,3244 +184,3315 @@ } } ], + "copyright": { + "statement": "Copyright \u00a9 2018 the Author(s). Published by PNAS.", + "status": true + }, + "keywords": [ + { + "keyString": "Alzheimer\u2019s disease", + "keySystem": "misc" + }, + { + "keyString": "whole-genome sequencing", + "keySystem": "misc" + }, + { + "keyString": "GWAS", + "keySystem": "misc" + }, + { + "keyString": "risk variant", + "keySystem": "misc" + }, + { + "keyString": "immune", + "keySystem": "misc" + } + ], + "openAccess": { + "license": "This open access article is distributed under Creative Commons Attribution-NonCommercial-NoDerivatives License 4.0 (CC BY-NC-ND).", + "licenseURL": "https://creativecommons.org/licenses/by-nc-nd/4.0/", + "open": true + }, "otherContributor": [ { - "role": "author non-byline", "contrib": { "name": { - "surname": "Saykin", - "given_name": "Andrew J." + "given_name": "Andrew J.", + "surname": "Saykin" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Toga", - "given_name": "Arthur W." + "given_name": "Arthur W.", + "surname": "Toga" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Borowski", - "given_name": "Bret" + "given_name": "Bret", + "surname": "Borowski" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Ward", - "given_name": "Chad" + "given_name": "Chad", + "surname": "Ward" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "DeCarli", - "given_name": "Charles" + "given_name": "Charles", + "surname": "DeCarli" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Mathis", - "given_name": "Chet" + "given_name": "Chet", + "surname": "Mathis" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Jack", - "given_name": "Clifford R." + "given_name": "Clifford R.", + "surname": "Jack" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Harvey", - "given_name": "Danielle" + "given_name": "Danielle", + "surname": "Harvey" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Holtzman", - "given_name": "David" + "given_name": "David", + "surname": "Holtzman" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Jones", - "given_name": "David" + "given_name": "David", + "surname": "Jones" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Gessert", - "given_name": "Devon" + "given_name": "Devon", + "surname": "Gessert" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Lilly", - "given_name": "Eli" + "given_name": "Eli", + "surname": "Lilly" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Reiman", - "given_name": "Eric M." + "given_name": "Eric M.", + "surname": "Reiman" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Franklin", - "given_name": "Erin" + "given_name": "Erin", + "surname": "Franklin" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Hefti", - "given_name": "Franz" + "given_name": "Franz", + "surname": "Hefti" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Sorensen", - "given_name": "Greg" + "given_name": "Greg", + "surname": "Sorensen" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Jimenez", - "given_name": "Gustavo" + "given_name": "Gustavo", + "surname": "Jimenez" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Fillit", - "given_name": "Howard" + "given_name": "Howard", + "surname": "Fillit" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Gunter", - "given_name": "Jeff" + "given_name": "Jeff", + "surname": "Gunter" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Salazar", - "given_name": "Jennifer" + "given_name": "Jennifer", + "surname": "Salazar" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Hsiao", - "given_name": "John" + "given_name": "John", + "surname": "Hsiao" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Morris", - "given_name": "John" + "given_name": "John", + "surname": "Morris" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Trojanowki", - "given_name": "John Q." + "given_name": "John Q.", + "surname": "Trojanowki" } - 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"role": "author non-byline", "contrib": { "name": { - "surname": "Nho", - "given_name": "Kwangsik" + "given_name": "Kwangsik", + "surname": "Nho" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Beckett", - "given_name": "Laurel" + "given_name": "Laurel", + "surname": "Beckett" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Thal", - "given_name": "Lean" + "given_name": "Lean", + "surname": "Thal" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Thal", - "given_name": "Leon" + "given_name": "Leon", + "surname": "Thal" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Shaw", - "given_name": "Leslie M." + "given_name": "Leslie M.", + "surname": "Shaw" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - 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"surname": "Nam", - "given_name": "Ki Won" + "given_name": "Ki Won", + "surname": "Nam" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Martin", - "given_name": "Kim" + "given_name": "Kim", + "surname": "Martin" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Poki-Walker", - "given_name": "Kim" + "given_name": "Kim", + "surname": "Poki-Walker" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Johnson", - "given_name": "Kris" + "given_name": "Kris", + "surname": "Johnson" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Fargher", - "given_name": "Kristin" + "given_name": "Kristin", + "surname": "Fargher" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Lipowski", - "given_name": "Kristine" + "given_name": "Kristine", + "surname": "Lipowski" } - 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} + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Silbert", - "given_name": "Lisa C." + "given_name": "Lisa C.", + "surname": "Silbert" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Ravdin", - "given_name": "Lisa" + "given_name": "Lisa", + "surname": "Ravdin" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Schneider", - "given_name": "Lon S." + "given_name": "Lon S.", + "surname": "Schneider" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Daiello", - "given_name": "Lori A." + "given_name": "Lori A.", + "surname": "Daiello" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Ismail", - "given_name": "M. Saleem" + "given_name": "M. Saleem", + "surname": "Ismail" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Seltzer", - "given_name": "Marc" + "given_name": "Marc", + "surname": "Seltzer" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Mesulam", - "given_name": "Marek-Marsel" + "given_name": "Marek-Marsel", + "surname": "Mesulam" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Carroll", - "given_name": "Maria" + "given_name": "Maria", + "surname": "Carroll" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Kataki", - "given_name": "Maria" + "given_name": "Maria", + "surname": "Kataki" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Greig-Custo", - "given_name": "Maria T." + "given_name": "Maria T.", + "surname": "Greig-Custo" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Love", - "given_name": "Marissa Natelson" + "given_name": "Marissa Natelson", + "surname": "Love" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Mintun", - "given_name": "Mark A." + "given_name": "Mark A.", + "surname": "Mintun" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Farlow", - "given_name": "Martin R." + "given_name": "Martin R.", + "surname": "Farlow" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Sadowski", - "given_name": "Martin" + "given_name": "Martin", + "surname": "Sadowski" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Creech", - "given_name": "Mary L." + "given_name": "Mary L.", + "surname": "Creech" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Hynes", - "given_name": "Mary L." + "given_name": "Mary L.", + "surname": "Hynes" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Quiceno", - "given_name": "Mary" + "given_name": "Mary", + "surname": "Quiceno" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Oakley", - "given_name": "MaryAnn" + "given_name": "MaryAnn", + "surname": "Oakley" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Becerra", - "given_name": "Mauricio" + "given_name": "Mauricio", + "surname": "Becerra" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Witbracht", - "given_name": "Megan" + "given_name": "Megan", + "surname": "Witbracht" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Keltz", - "given_name": "Melanie" + "given_name": "Melanie", + "surname": "Keltz" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Lamar", - "given_name": "Melissa" + "given_name": "Melissa", + "surname": "Lamar" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Yang", - "given_name": "Mia" + "given_name": "Mia", + "surname": "Yang" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Borrie", - "given_name": "Michael" + "given_name": "Michael", + "surname": "Borrie" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Lin", - "given_name": "Michael" + "given_name": "Michael", + "surname": "Lin" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Assaly", - "given_name": "Michele" + "given_name": "Michele", + "surname": "Assaly" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Rainka", - "given_name": "Michelle" + "given_name": "Michelle", + "surname": "Rainka" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Dang", - "given_name": "Mimi" + "given_name": "Mimi", + "surname": "Dang" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Sheikh", - "given_name": "Mohammed O." + "given_name": "Mohammed O.", + "surname": "Sheikh" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Gaikwad", - "given_name": "Mrunalini" + "given_name": "Mrunalini", + "surname": "Gaikwad" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Chowdhury", - "given_name": "Munir" + "given_name": "Munir", + "surname": "Chowdhury" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Trncic", - "given_name": "Nadira" + "given_name": "Nadira", + "surname": "Trncic" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Johnson", - "given_name": "Nancy" + "given_name": "Nancy", + "surname": "Johnson" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Kowalksi", - "given_name": "Nancy" + "given_name": "Nancy", + "surname": "Kowalksi" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Pacini", - "given_name": "Nathaniel" + "given_name": "Nathaniel", + "surname": "Pacini" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Kowall", - "given_name": "Neil" + "given_name": "Neil", + "surname": "Kowall" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Graff-Radford", - "given_name": "Neill R" + "given_name": "Neill R", + "surname": "Graff-Radford" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Relkin", - "given_name": "Norman" + "given_name": "Norman", + "surname": "Relkin" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Oyonumo", - "given_name": "Ntekim E." + "given_name": "Ntekim E.", + "surname": "Oyonumo" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Pomara", - "given_name": "Nunzio" + "given_name": "Nunzio", + "surname": "Pomara" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "James", - "given_name": "Olga" + "given_name": "Olga", + "surname": "James" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Ogunlana", - "given_name": "Olu" + "given_name": "Olu", + "surname": "Ogunlana" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Lopez", - "given_name": "Oscar L." + "given_name": "Oscar L.", + "surname": "Lopez" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Carmichael", - "given_name": "Owen" + "given_name": "Owen", + "surname": "Carmichael" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Doraiswamy", - "given_name": "P. Murali" + "given_name": "P. Murali", + "surname": "Doraiswamy" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Fatica", - "given_name": "Parianne" + "given_name": "Parianne", + "surname": "Fatica" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Johnson", - "given_name": "Patricia Lynn" + "given_name": "Patricia Lynn", + "surname": "Johnson" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Samuels", - "given_name": "Patricia" + "given_name": "Patricia", + "surname": "Samuels" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Malloy", - "given_name": "Paul" + "given_name": "Paul", + "surname": "Malloy" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Ogrocki", - "given_name": "Paula" + "given_name": "Paula", + "surname": "Ogrocki" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Maillard", - "given_name": "Pauline" + "given_name": "Pauline", + "surname": "Maillard" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Hardy", - "given_name": "Peter" + "given_name": "Peter", + "surname": "Hardy" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Tariot", - "given_name": "Pierre" + "given_name": "Pierre", + "surname": "Tariot" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Lu", - "given_name": "Po H." + "given_name": "Po H.", + "surname": "Lu" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Varma", - "given_name": "Pradeep" + "given_name": "Pradeep", + "surname": "Varma" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Doody", - "given_name": "Rachelle S." + "given_name": "Rachelle S.", + "surname": "Doody" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Carter", - "given_name": "Raina" + "given_name": "Raina", + "surname": "Carter" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Shah", - "given_name": "Raj C." + "given_name": "Raj C.", + "surname": "Shah" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Griffith", - "given_name": "Randall" + "given_name": "Randall", + "surname": "Griffith" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Yeh", - "given_name": "Randy" + "given_name": "Randy", + "surname": "Yeh" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Duara", - "given_name": "Ranjan" + "given_name": "Ranjan", + "surname": "Duara" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Tarawneh", - "given_name": "Rawan" + "given_name": "Rawan", + "surname": "Tarawneh" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Turner", - "given_name": "Raymond Scott" + "given_name": "Raymond Scott", + "surname": "Turner" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Hernando", - "given_name": "Raymundo" + "given_name": "Raymundo", + "surname": "Hernando" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Sperling", - "given_name": "Reisa A." + "given_name": "Reisa A.", + "surname": "Sperling" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Carson", - "given_name": "Richard E." + "given_name": "Richard E.", + "surname": "Carson" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "El Khouli", - "given_name": "Riham" + "given_name": "Riham", + "surname": "El Khouli" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Santulli", - "given_name": "Robert B." + "given_name": "Robert B.", + "surname": "Santulli" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Killiany", - "given_name": "Ronald" + "given_name": "Ronald", + "surname": "Killiany" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Rodriguez", - "given_name": "Rosemarie" + "given_name": "Rosemarie", + "surname": "Rodriguez" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Swerdlow", - "given_name": "Russell H." + "given_name": "Russell H.", + "surname": "Swerdlow" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Borges-Neto", - "given_name": "Salvador" + "given_name": "Salvador", + "surname": "Borges-Neto" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Black", - "given_name": "Sandra" + "given_name": "Sandra", + "surname": "Black" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Weintraub", - "given_name": "Sandra" + "given_name": "Sandra", + "surname": "Weintraub" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Asthana", - "given_name": "Sanjay" + "given_name": "Sanjay", + "surname": "Asthana" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Vaishnavi", - "given_name": "Sanjeev" + "given_name": "Sanjeev", + "surname": "Vaishnavi" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Dolen", - "given_name": "Sara" + "given_name": "Sara", + "surname": "Dolen" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Mason", - "given_name": "Sara S." + "given_name": "Sara S.", + "surname": "Mason" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Kremen", - "given_name": "Sarah" + "given_name": "Sarah", + "surname": "Kremen" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Herring", - "given_name": "Scott" + "given_name": "Scott", + "surname": "Herring" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Sirrel", - "given_name": "Sherye A." + "given_name": "Sherye A.", + "surname": "Sirrel" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Kittur", - "given_name": "Smita" + "given_name": "Smita", + "surname": "Kittur" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Pawluczyk", - "given_name": "Sonia" + "given_name": "Sonia", + "surname": "Pawluczyk" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Schneider", - "given_name": "Stacy" + "given_name": "Stacy", + "surname": "Schneider" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Kielb", - "given_name": "Stephanie" + "given_name": "Stephanie", + "surname": "Kielb" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Reeder", - "given_name": "Stephanie" + "given_name": "Stephanie", + "surname": "Reeder" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Correia", - "given_name": "Stephen" + "given_name": "Stephen", + "surname": "Correia" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Pasternack", - "given_name": "Stephen" + "given_name": "Stephen", + "surname": "Pasternack" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Pasternak", - "given_name": "Stephen" + "given_name": "Stephen", + "surname": "Pasternak" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Salloway", - "given_name": "Stephen" + "given_name": "Stephen", + "surname": "Salloway" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Johnson", - "given_name": "Sterling" + "given_name": "Sterling", + "surname": "Johnson" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Chao", - "given_name": "Steven" + "given_name": "Steven", + "surname": "Chao" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Arnold", - "given_name": "Steven E." + "given_name": "Steven E.", + "surname": "Arnold" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Schultz", - "given_name": "Susan K." + "given_name": "Susan K.", + "surname": "Schultz" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Rountree", - "given_name": "Susan" + "given_name": "Susan", + "surname": "Rountree" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Lee", - "given_name": "T-Y" + "given_name": "T-Y", + "surname": "Lee" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Wong", - "given_name": "Terence Z." + "given_name": "Terence Z.", + "surname": "Wong" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Villena", - "given_name": "Teresa" + "given_name": "Teresa", + "surname": "Villena" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Obisesan", - "given_name": "Thomas O." + "given_name": "Thomas O.", + "surname": "Obisesan" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Pavlik", - "given_name": "Valory" + "given_name": "Valory", + "surname": "Pavlik" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Bates", - "given_name": "Vernice" + "given_name": "Vernice", + "surname": "Bates" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Sossi", - "given_name": "Vesna" + "given_name": "Vesna", + "surname": "Sossi" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Shibley", - "given_name": "Victoria" + "given_name": "Victoria", + "surname": "Shibley" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Brooks", - "given_name": "William M." + "given_name": "William M.", + "surname": "Brooks" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Pavlosky", - "given_name": "William" + "given_name": "William", + "surname": "Pavlosky" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Stern", - "given_name": "Yaakov" + "given_name": "Yaakov", + "surname": "Stern" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Simon", - "given_name": "Adam" + "given_name": "Adam", + "surname": "Simon" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Dongre", - "given_name": "Ashok" + "given_name": "Ashok", + "surname": "Dongre" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Dean", - "given_name": "Bob" + "given_name": "Bob", + "surname": "Dean" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Navia", - "given_name": "Brad" + "given_name": "Brad", + "surname": "Navia" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Spellman", - "given_name": "Dan" + "given_name": "Dan", + "surname": "Spellman" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Lee", - "given_name": "David" + "given_name": "David", + "surname": "Lee" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Shera", - "given_name": "David" + "given_name": "David", + "surname": "Shera" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Siemers", - "given_name": "Eric" + "given_name": "Eric", + "surname": "Siemers" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Pickering", - "given_name": "Eve" + "given_name": "Eve", + "surname": "Pickering" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Swenson", - "given_name": "Frank" + "given_name": "Frank", + "surname": "Swenson" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Immerman", - "given_name": "Fred" + "given_name": "Fred", + "surname": "Immerman" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Nomikos", - "given_name": "George" + "given_name": "George", + "surname": "Nomikos" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Soares", - "given_name": "Holly" + "given_name": "Holly", + "surname": "Soares" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Wan", - "given_name": "Hong" + "given_name": "Hong", + "surname": "Wan" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Seeburger", - "given_name": "Jeff" + "given_name": "Jeff", + "surname": "Seeburger" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Waring", - "given_name": "Jeff" + "given_name": "Jeff", + "surname": "Waring" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Trojanowski", - "given_name": "John" + "given_name": "John", + "surname": "Trojanowski" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Siuciak", - "given_name": "Judy" + "given_name": "Judy", + "surname": "Siuciak" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Duffin", - "given_name": "Kevin" + "given_name": "Kevin", + "surname": "Duffin" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Shaw", - "given_name": "Les" + "given_name": "Les", + "surname": "Shaw" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Wang", - "given_name": "Li-San" + "given_name": "Li-San", + "surname": "Wang" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Thambisetty", - "given_name": "Madhav" + "given_name": "Madhav", + "surname": "Thambisetty" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Walton", - "given_name": "Marc" + "given_name": "Marc", + "surname": "Walton" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Savage", - "given_name": "Mary" + "given_name": "Mary", + "surname": "Savage" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Ferm", - "given_name": "Mats" + "given_name": "Mats", + "surname": "Ferm" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Kuhn", - "given_name": "Max" + "given_name": "Max", + "surname": "Kuhn" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Buckholtz", - "given_name": "Neil" + "given_name": "Neil", + "surname": "Buckholtz" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Zagouras", - "given_name": "Panos" + "given_name": "Panos", + "surname": "Zagouras" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Cole", - "given_name": "Patricia" + "given_name": "Patricia", + "surname": "Cole" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Hendrickson", - "given_name": "Ron" + "given_name": "Ron", + "surname": "Hendrickson" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Xie", - "given_name": "Sharon" + "given_name": "Sharon", + "surname": "Xie" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Allauzen", - "given_name": "Sophie" + "given_name": "Sophie", + "surname": "Allauzen" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Koroshetz", - "given_name": "Walter" + "given_name": "Walter", + "surname": "Koroshetz" } - } + }, + "role": "author non-byline" }, { - "role": "author non-byline", "contrib": { "name": { - "surname": "Potter", - "given_name": "William" + "given_name": "William", + "surname": "Potter" } - } + }, + "role": "author non-byline" } ], - "title": { - "textEnglish": "Identification of genetic risk factors in the Chinese population implicates a role of immune system in Alzheimer\u2019s disease pathogenesis" + "pagination": { + "firstPage": "1697", + "lastPage": "1706", + "pageCount": "10", + "pageRange": "1697-1706" }, - "abstract": { - "textEnglish": "Alzheimer\u2019s disease (AD) is an age-related neurodegenerative disease. Genome-wide association studies predominately focusing on Caucasian populations have identified risk loci and genes associated with AD; the majority of these variants reside in noncoding regions with unclear functions. Here, we report a whole-genome sequencing study for AD in the Chinese population. Other than the APOE locus, we identified common variants in GCH1 and KCNJ15 that show suggestive associations with AD. For these two risk variants, an association with AD or advanced onset of disease can be observed in non-Asian AD cohorts. An association study of risk variants with expression data revealed their modulatory effects on immune signatures, linking the potential roles of these genes with immune-related pathways during AD pathogenesis." + "persistentIDs": [ + { + "DOI": "10.1073/pnas.1715554115" + } + ], + "pubDate": { + "electrDate": "2018-02-05", + "printDate": "2018-02-20" + }, + "publication": { + "ISSN": [ + { + "issnString": "0027-8424", + "pubtype": "ppub" + }, + { + "issnString": "1091-6490", + "pubtype": "epub" + } + ], + "issueNum": "8", + "pubName": "Proceedings of the National Academy of Sciences", + "pubYear": "2018", + "publisher": "National Academy of Sciences", + "volumeNum": "115" + }, + "publisherIDs": [ + { + "Identifier": "201715554", + "attribute": "publisher-id" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ "KY Chan, , Epidemiology of Alzheimer\u2019s disease and other forms of dementia in China, 1990-2010: A systematic review and analysis. Lancet; Global Health Epidemiology Reference Group (GHERG) 381, 2016\u20132023 (2013).", @@ -3546,35 +3574,7 @@ "E Masliah, W Dumaop, D Galasko, P Desplats, Distinctive patterns of DNA methylation associated with Parkinson disease: Identification of concordant epigenetic changes in brain and peripheral blood leukocytes. Epigenetics 8, 1030\u20131038 (2013).", "NA Bowden, , Preliminary investigation of gene expression profiles in peripheral blood lymphocytes in schizophrenia. Schizophr Res 82, 175\u2013183 (2006)." ], - "keywords": [ - { - "keyString": "Alzheimer\u2019s disease", - "keySystem": "misc" - }, - { - "keyString": "whole-genome sequencing", - "keySystem": "misc" - }, - { - "keyString": "GWAS", - "keySystem": "misc" - }, - { - "keyString": "risk variant", - "keySystem": "misc" - }, - { - "keyString": "immune", - "keySystem": "misc" - } - ], - "copyright": { - "status": true, - "statement": "Copyright \u00a9 2018 the Author(s). Published by PNAS." - }, - "openAccess": { - "open": true, - "license": "This open access article is distributed under Creative Commons Attribution-NonCommercial-NoDerivatives License 4.0 (CC BY-NC-ND).", - "licenseURL": "https://creativecommons.org/licenses/by-nc-nd/4.0/" + "title": { + "textEnglish": "Identification of genetic risk factors in the Chinese population implicates a role of immune system in Alzheimer\u2019s disease pathogenesis" } } diff --git a/tests/stubdata/output/jats_spie_opten_1.OE.62.4.048103.json b/tests/stubdata/output/jats_spie_opten_1.OE.62.4.048103.json index 0d7baa9..63c245d 100644 --- a/tests/stubdata/output/jats_spie_opten_1.OE.62.4.048103.json +++ b/tests/stubdata/output/jats_spie_opten_1.OE.62.4.048103.json @@ -1,97 +1,127 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" + "abstract": { + "textEnglish": "Within the last decades, a large number of techniques for contrast enhancement has been proposed. There are some comparisons of such algorithms for few images and figures of merit. However, many of these figures of merit cannot assess usability of altered image content for specific tasks, such as object recognition. In this work, the effect of contrast enhancement algorithms is evaluated by means of the triangle orientation discrimination (TOD), which is a current method for imager performance assessment. The conventional TOD approach requires observers to recognize equilateral triangles pointing in four different directions, whereas here convolutional neural network models are used for the classification task. These models are trained by artificial images with single triangles. Many methods for contrast enhancement highly depend on the content of the entire image. Therefore, the images are superimposed over natural backgrounds with varying standard deviations to provide different signal-to-background ratios. Then, these images are degraded by Gaussian blur and noise representing degradational camera effects and sensor noise. Different algorithms, such as the contrast-limited adaptive histogram equalization or local range modification, are applied. Then accuracies of the trained models on these images are compared for different contrast enhancement algorithms. Accuracy gains for low signal-to-background ratios and sufficiently large triangles are found, whereas impairments are found for high signal-to-background ratios and small triangles. A high generalization ability of our TOD model is found from the similar accuracies for several image databases used for backgrounds. Finally, implications of replacing triangles with real target signatures when using such advanced digital signal processing algorithms are discussed. The results are a step toward the assessment of those algorithms for generic target recognition." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "aff1", + "affPubRaw": "Fraunhofer Institute of Optronics, System Technologies and Image Exploitation, Ettlingen, Germany" + } + ], + "attrib": { + "email": "daniel.wegner@iosb.fraunhofer.de" + }, + "name": { + "given_name": "Daniel", + "surname": "Wegner" + } + }, + { + "affiliation": [ + { + "affPubID": "aff1", + "affPubRaw": "Fraunhofer Institute of Optronics, System Technologies and Image Exploitation, Ettlingen, Germany" + } + ], + "attrib": { + "email": "stefan.kessler@iosb.fraunhofer.de" + }, + "name": { + "given_name": "Stefan", + "surname": "Ke\u00dfler" + } + } + ], + "copyright": { + "statement": "\u00a9 The Authors. Published by SPIE under a Creative Commons Attribution 4.0 International License. Distribution or reproduction of this work in whole or in part requires full attribution of the original publication, including its DOI.", + "status": true }, "editorialHistory": { + "acceptedDate": "2023-03-24", "receivedDates": [ "2022-12-08" - ], - "acceptedDate": "2023-03-24" - }, - "pubDate": { - "electrDate": "2023-04-20", - "printDate": "2023-04-01" - }, - "publication": { - "pubName": "Optical Engineering", - "publisher": "Society of Photo-Optical Instrumentation Engineers", - "issueNum": "4", - "volumeNum": "62", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "0091-3286" - }, - { - "pubtype": "epub", - "issnString": "1560-2303" - } ] }, - "persistentIDs": [ + "keywords": [ { - "DOI": "10.1117/1.OE.62.4.048103" - } - ], - "publisherIDs": [ + "keyString": "advanced digital signal processing", + "keySystem": "misc" + }, { - "attribute": "manuscript", - "Identifier": "OE-20221420G" + "keyString": "convolutional neural networks", + "keySystem": "misc" + }, + { + "keyString": "image contrast enhancement", + "keySystem": "misc" + }, + { + "keyString": "imager assessment", + "keySystem": "misc" }, { - "attribute": "publisher-id", - "Identifier": "20221420G" + "keyString": "method comparison", + "keySystem": "misc" + }, + { + "keyString": "triangle orientation discrimination", + "keySystem": "misc" } ], + "openAccess": { + "open": true + }, "pagination": { "firstPage": "048103", "lastPage": "048103", "pageCount": "20", "pageRange": "048103-048103" }, - "authors": [ + "persistentIDs": [ { - "name": { - "surname": "Wegner", - "given_name": "Daniel" + "DOI": "10.1117/1.OE.62.4.048103" + } + ], + "pubDate": { + "electrDate": "2023-04-20", + "printDate": "2023-04-01" + }, + "publication": { + "ISSN": [ + { + "issnString": "0091-3286", + "pubtype": "ppub" }, - "affiliation": [ - { - "affPubRaw": "Fraunhofer Institute of Optronics, System Technologies and Image Exploitation, Ettlingen, Germany", - "affPubID": "aff1" - } - ], - "attrib": { - "email": "daniel.wegner@iosb.fraunhofer.de" + { + "issnString": "1560-2303", + "pubtype": "epub" } + ], + "issueNum": "4", + "pubName": "Optical Engineering", + "pubYear": "2023", + "publisher": "Society of Photo-Optical Instrumentation Engineers", + "volumeNum": "62" + }, + "publisherIDs": [ + { + "Identifier": "OE-20221420G", + "attribute": "manuscript" }, { - "name": { - "surname": "Ke\u00dfler", - "given_name": "Stefan" - }, - "affiliation": [ - { - "affPubRaw": "Fraunhofer Institute of Optronics, System Technologies and Image Exploitation, Ettlingen, Germany", - "affPubID": "aff1" - } - ], - "attrib": { - "email": "stefan.kessler@iosb.fraunhofer.de" - } + "Identifier": "20221420G", + "attribute": "publisher-id" } ], - "title": { - "textEnglish": "Comparison of algorithms for contrast enhancement based on triangle orientation discrimination assessments by convolutional neural networks" - }, - "abstract": { - "textEnglish": "Within the last decades, a large number of techniques for contrast enhancement has been proposed. There are some comparisons of such algorithms for few images and figures of merit. However, many of these figures of merit cannot assess usability of altered image content for specific tasks, such as object recognition. In this work, the effect of contrast enhancement algorithms is evaluated by means of the triangle orientation discrimination (TOD), which is a current method for imager performance assessment. The conventional TOD approach requires observers to recognize equilateral triangles pointing in four different directions, whereas here convolutional neural network models are used for the classification task. These models are trained by artificial images with single triangles. Many methods for contrast enhancement highly depend on the content of the entire image. Therefore, the images are superimposed over natural backgrounds with varying standard deviations to provide different signal-to-background ratios. Then, these images are degraded by Gaussian blur and noise representing degradational camera effects and sensor noise. Different algorithms, such as the contrast-limited adaptive histogram equalization or local range modification, are applied. Then accuracies of the trained models on these images are compared for different contrast enhancement algorithms. Accuracy gains for low signal-to-background ratios and sufficiently large triangles are found, whereas impairments are found for high signal-to-background ratios and small triangles. A high generalization ability of our TOD model is found from the similar accuracies for several image databases used for backgrounds. Finally, implications of replacing triangles with real target signatures when using such advanced digital signal processing algorithms are discussed. The results are a step toward the assessment of those algorithms for generic target recognition." + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " P. Bijl and J. M.Valeton, \u201cTriangle orientation discrimination: the alternative to minimum resolvable temperature difference and minimum resolvable contrast,\u201d Opt. Eng.37(7), 1976\u20131983 (1998).https://doi.org/10.1117/1.601904 ", @@ -164,37 +194,7 @@ " B. N. Anoop , P. E.Ameenudeen and J.Joseph, \u201cA meta-analysis of contrast measures used for the performance evaluation of histogram equalization based image enhancement techniques,\u201d in 9th Int. Conf. Comput., Commun. and Netw. Technol. (ICCCNT), pp. 1\u20136 (2018).https://doi.org/10.1109/ICCCNT.2018.8494069 ", " S. V. Renuka , D. R.Edla and J.Joseph, \u201cAn objective measure for assessing the quality of contrast enhancement on magnetic resonance images,\u201d J. King Saud Univ. \u2013 Comput. Inf. Sci.34(10, Part B), 9732\u20139744 (2021).https://doi.org/10.1016/j.jksuci.2021.12.005 " ], - "keywords": [ - { - "keyString": "advanced digital signal processing", - "keySystem": "misc" - }, - { - "keyString": "convolutional neural networks", - "keySystem": "misc" - }, - { - "keyString": "image contrast enhancement", - "keySystem": "misc" - }, - { - "keyString": "imager assessment", - "keySystem": "misc" - }, - { - "keyString": "method comparison", - "keySystem": "misc" - }, - { - "keyString": "triangle orientation discrimination", - "keySystem": "misc" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 The Authors. Published by SPIE under a Creative Commons Attribution 4.0 International License. Distribution or reproduction of this work in whole or in part requires full attribution of the original publication, including its DOI." - }, - "openAccess": { - "open": true + "title": { + "textEnglish": "Comparison of algorithms for contrast enhancement based on triangle orientation discrimination assessments by convolutional neural networks" } } diff --git a/tests/stubdata/output/jats_spie_opten_1.OE.62.4.066101.json b/tests/stubdata/output/jats_spie_opten_1.OE.62.4.066101.json index ab0692d..18d2885 100644 --- a/tests/stubdata/output/jats_spie_opten_1.OE.62.4.066101.json +++ b/tests/stubdata/output/jats_spie_opten_1.OE.62.4.066101.json @@ -1,129 +1,67 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2023-03-26" - ], - "revisedDates": [ - "2023-05-16" - ], - "acceptedDate": "2023-05-31" - }, - "pubDate": { - "electrDate": "2023-06-12", - "printDate": "2023-06-01" - }, - "publication": { - "pubName": "Optical Engineering", - "publisher": "Society of Photo-Optical Instrumentation Engineers", - "issueNum": "6", - "volumeNum": "62", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "0091-3286" - }, - { - "pubtype": "epub", - "issnString": "1560-2303" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1117/1.OE.62.6.066101" - } - ], - "publisherIDs": [ - { - "attribute": "manuscript", - "Identifier": "OE-20230249G" - }, - { - "attribute": "publisher-id", - "Identifier": "20230249G" - } - ], - "pagination": { - "firstPage": "066101", - "lastPage": "066101", - "pageCount": "9", - "pageRange": "066101-066101" + "abstract": { + "textEnglish": "High power fiber-coupled diode lasers are widely applied in laser material processing. Based on the commercial diode laser stacks, a comprehensive study of fiber-coupled diode lasers was presented using visualized beam shaping simulations. And then in experiment, refraction optical beam shaping, polarization multiplexing, wavelength multiplexing, and fiber coupling were used to produce a 4.08 kW output from an optical fiber with core diameter of 800 \u03bcm and NA of 0.2. An average fiber coupling efficiency about 95% was obtained, which was in good agreement with the simulation." }, "authors": [ { - "name": { - "surname": "Liao", - "given_name": "Jingxing" - }, "affiliation": [ { - "affPubRaw": "China National Institute of Standardization, Beijing, China", - "affPubID": "aff1" + "affPubID": "aff1", + "affPubRaw": "China National Institute of Standardization, Beijing, China" } ], "attrib": { "email": "liaojx@cnis.ac.cn" + }, + "name": { + "given_name": "Jingxing", + "surname": "Liao" } }, { - "name": { - "surname": "Feng", - "given_name": "Lei" - }, "affiliation": [ { - "affPubRaw": "China National Institute of Standardization, Beijing, China", - "affPubID": "aff1" + "affPubID": "aff1", + "affPubRaw": "China National Institute of Standardization, Beijing, China" } ], "attrib": { "email": "fenglei@cnis.ac.cn" + }, + "name": { + "given_name": "Lei", + "surname": "Feng" } }, { - "name": { - "surname": "Yang", - "given_name": "Jingna" - }, "affiliation": [ { - "affPubRaw": "China National Institute of Standardization, Beijing, China", - "affPubID": "aff1" + "affPubID": "aff1", + "affPubRaw": "China National Institute of Standardization, Beijing, China" } ], "attrib": { "email": "yangjn@cnis.ac.cn" + }, + "name": { + "given_name": "Jingna", + "surname": "Yang" } } ], - "title": { - "textEnglish": "High power fiber-coupled diode laser based on beam shaping simulation" + "copyright": { + "statement": "\u00a9 2023 Society of Photo-Optical Instrumentation Engineers (SPIE)", + "status": true }, - "abstract": { - "textEnglish": "High power fiber-coupled diode lasers are widely applied in laser material processing. Based on the commercial diode laser stacks, a comprehensive study of fiber-coupled diode lasers was presented using visualized beam shaping simulations. And then in experiment, refraction optical beam shaping, polarization multiplexing, wavelength multiplexing, and fiber coupling were used to produce a 4.08 kW output from an optical fiber with core diameter of 800 \u03bcm and NA of 0.2. An average fiber coupling efficiency about 95% was obtained, which was in good agreement with the simulation." + "editorialHistory": { + "acceptedDate": "2023-05-31", + "receivedDates": [ + "2023-03-26" + ], + "revisedDates": [ + "2023-05-16" + ] }, - "references": [ - " C. M. Stickley et al. , \u201cThe future of high-efficiency diode lasers,\u201d Proc. SPIE5991, 59911O (2006).PSISDG0277-786Xhttps://doi.org/10.1117/12.639142 ", - " C. M. Stickley et al. , \u201cOverview of progress in super high efficiency diodes for pumping high energy lasers,\u201d Proc. SPIE6104, 610405 (2006).PSISDG0277-786Xhttps://doi.org/10.1117/12.640448 ", - " F. Bachmann , \u201cGoals and status of the German national research initiative BRIOLAS (brilliant diode lasers),\u201d Proc. SPIE6456, 645608 (2007).PSISDG0277-786Xhttps://doi.org/10.1117/12.700146 ", - " F. G. Bachmann , \u201cStatus and results of the German national diode laser research project \u201cModular Diode Laser Systems\u201d (MDS),\u201d Proc. SPIE4831, 14\u201320 (2003).PSISDG0277-786Xhttps://doi.org/10.1117/12.497969 ", - " P. Crump et al. , \u201cDevelopment of high-power diode lasers with beam parameter product below 2 mm\u00d7mrad within the BRIDLE project,\u201d Proc. SPIE9348, 93480D (2015).PSISDG0277-786Xhttps://doi.org/10.1117/12.2077617 ", - " A. Unger et al. , \u201cThe BRIDLE project: high brilliance diode lasers for industrial applications,\u201d in High Power Diode Lasers and Systems Conf. (HPD), West Midlands, UK, pp. 28\u201329 (2013).https://doi.org/10.1109/HPD.2013.6706602 ", - " D. G. Matthews et al. , \u201cA 15-kW fiber-coupled diode laser for pumping applications,\u201d Proc. SPIE8241, 824103 (2012).PSISDG0277-786Xhttps://doi.org/10.1117/12.906464 ", - " J. Malchus et al. , \u201cA 25kW fiber-coupled diode laser for pumping applications,\u201d Proc. SPIE8965, 89650B (2014).PSISDG0277-786Xhttps://doi.org/10.1117/12.2039110 ", - " J. Malchus et al. , \u201cA 40kW fiber-coupled diode laser for material processing and pumping applications,\u201d Proc. SPIE9348, 934803 (2015).PSISDG0277-786Xhttps://doi.org/10.1117/12.2083909 ", - " Z. Dong et al. , \u201cSimulation for fiber-coupled diode lasers by considering discreteness in propagation angles of individual emitters,\u201d Opt. Laser Technol.132, 106500 (2020).OLTCAS0030-3992https://doi.org/10.1016/j.optlastec.2020.106500 ", - " Z. Wang et al. , \u201cFiber coupled diode laser beam parameter product calculation and rules for optimized design,\u201d Proc. SPIE7918, 791809 (2011).PSISDG0277-786Xhttps://doi.org/10.1117/12.875386 " - ], "keywords": [ { "keyString": "beam shaping", @@ -142,11 +80,73 @@ "keySystem": "misc" } ], - "copyright": { - "status": true, - "statement": "\u00a9 2023 Society of Photo-Optical Instrumentation Engineers (SPIE)" - }, "openAccess": { "license": "0091-3286/2023/$28.00 \u00a9 2023 SPIE" + }, + "pagination": { + "firstPage": "066101", + "lastPage": "066101", + "pageCount": "9", + "pageRange": "066101-066101" + }, + "persistentIDs": [ + { + "DOI": "10.1117/1.OE.62.6.066101" + } + ], + "pubDate": { + "electrDate": "2023-06-12", + "printDate": "2023-06-01" + }, + "publication": { + "ISSN": [ + { + "issnString": "0091-3286", + "pubtype": "ppub" + }, + { + "issnString": "1560-2303", + "pubtype": "epub" + } + ], + "issueNum": "6", + "pubName": "Optical Engineering", + "pubYear": "2023", + "publisher": "Society of Photo-Optical Instrumentation Engineers", + "volumeNum": "62" + }, + "publisherIDs": [ + { + "Identifier": "OE-20230249G", + "attribute": "manuscript" + }, + { + "Identifier": "20230249G", + "attribute": "publisher-id" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + " C. M. Stickley et al. , \u201cThe future of high-efficiency diode lasers,\u201d Proc. SPIE5991, 59911O (2006).PSISDG0277-786Xhttps://doi.org/10.1117/12.639142 ", + " C. M. Stickley et al. , \u201cOverview of progress in super high efficiency diodes for pumping high energy lasers,\u201d Proc. SPIE6104, 610405 (2006).PSISDG0277-786Xhttps://doi.org/10.1117/12.640448 ", + " F. Bachmann , \u201cGoals and status of the German national research initiative BRIOLAS (brilliant diode lasers),\u201d Proc. SPIE6456, 645608 (2007).PSISDG0277-786Xhttps://doi.org/10.1117/12.700146 ", + " F. G. Bachmann , \u201cStatus and results of the German national diode laser research project \u201cModular Diode Laser Systems\u201d (MDS),\u201d Proc. SPIE4831, 14\u201320 (2003).PSISDG0277-786Xhttps://doi.org/10.1117/12.497969 ", + " P. Crump et al. , \u201cDevelopment of high-power diode lasers with beam parameter product below 2 mm\u00d7mrad within the BRIDLE project,\u201d Proc. SPIE9348, 93480D (2015).PSISDG0277-786Xhttps://doi.org/10.1117/12.2077617 ", + " A. Unger et al. , \u201cThe BRIDLE project: high brilliance diode lasers for industrial applications,\u201d in High Power Diode Lasers and Systems Conf. (HPD), West Midlands, UK, pp. 28\u201329 (2013).https://doi.org/10.1109/HPD.2013.6706602 ", + " D. G. Matthews et al. , \u201cA 15-kW fiber-coupled diode laser for pumping applications,\u201d Proc. SPIE8241, 824103 (2012).PSISDG0277-786Xhttps://doi.org/10.1117/12.906464 ", + " J. Malchus et al. , \u201cA 25kW fiber-coupled diode laser for pumping applications,\u201d Proc. SPIE8965, 89650B (2014).PSISDG0277-786Xhttps://doi.org/10.1117/12.2039110 ", + " J. Malchus et al. , \u201cA 40kW fiber-coupled diode laser for material processing and pumping applications,\u201d Proc. SPIE9348, 934803 (2015).PSISDG0277-786Xhttps://doi.org/10.1117/12.2083909 ", + " Z. Dong et al. , \u201cSimulation for fiber-coupled diode lasers by considering discreteness in propagation angles of individual emitters,\u201d Opt. Laser Technol.132, 106500 (2020).OLTCAS0030-3992https://doi.org/10.1016/j.optlastec.2020.106500 ", + " Z. Wang et al. , \u201cFiber coupled diode laser beam parameter product calculation and rules for optimized design,\u201d Proc. SPIE7918, 791809 (2011).PSISDG0277-786Xhttps://doi.org/10.1117/12.875386 " + ], + "title": { + "textEnglish": "High power fiber-coupled diode laser based on beam shaping simulation" } } diff --git a/tests/stubdata/output/jats_spie_spie_12.2690579.json b/tests/stubdata/output/jats_spie_spie_12.2690579.json index 755606f..2508411 100644 --- a/tests/stubdata/output/jats_spie_spie_12.2690579.json +++ b/tests/stubdata/output/jats_spie_spie_12.2690579.json @@ -1,96 +1,96 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "pubDate": { - "electrDate": "2023-06-15", - "printDate": "2023-06-15" + "abstract": { + "textEnglish": "This PDF file contains the front matter associated with SPIE Proceedings Volume 12512, including the Title Page, Copyright information, Table of Contents, and Conference Committee information." }, - "publication": { - "confName": "Defense + Commercial Sensing", - "publisher": "SPIE", - "issueNum": "None", - "volumeNum": "12512", - "pubYear": "2023", - "ISSN": [ - { - "issnString": "0277-786X" - } - ] + "copyright": { + "statement": "COPYRIGHT SPIE. 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Alex" - }, "affiliation": [ { - "affPubRaw": "MIT Lincoln Lab. (United States)", - "affPubID": "aff3" + "affPubID": "aff3", + "affPubRaw": "MIT Lincoln Lab. (United States)" } - ] - } + ], + "name": { + "given_name": "K. Alex", + "surname": "McIntosh" + } + }, + "role": "editor" } ], - "title": { - "textEnglish": "Front Matter: Volume 12512" + "pagination": { + "firstPage": "1251201", + "lastPage": "1251201-6", + "pageRange": "1251201-1251201-6" }, - "abstract": { - "textEnglish": "This PDF file contains the front matter associated with SPIE Proceedings Volume 12512, including the Title Page, Copyright information, Table of Contents, and Conference Committee information." + "persistentIDs": [ + { + "DOI": "10.1117/12.2690579" + } + ], + "pubDate": { + "electrDate": "2023-06-15", + "printDate": "2023-06-15" }, - "copyright": { - "status": true, - "statement": "COPYRIGHT SPIE. Downloading of the abstract is permitted for personal use only." + "publication": { + "ISSN": [ + { + "issnString": "0277-786X" + } + ], + "confName": "Defense + Commercial Sensing", + "issueNum": "None", + "pubYear": "2023", + "publisher": "SPIE", + "volumeNum": "12512" }, - "openAccess": { - "open": true + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "title": { + "textEnglish": "Front Matter: Volume 12512" } } diff --git a/tests/stubdata/output/jats_springer_EPJC_s10052-023-11699-1.json b/tests/stubdata/output/jats_springer_EPJC_s10052-023-11699-1.json index 2135de1..f7b7df9 100644 --- a/tests/stubdata/output/jats_springer_EPJC_s10052-023-11699-1.json +++ b/tests/stubdata/output/jats_springer_EPJC_s10052-023-11699-1.json @@ -1,44913 +1,44919 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2022-11-30" - ], - "acceptedDate": "2023-01-27" - }, - "pubDate": { - "electrDate": "2023-07-00" - }, - "publication": { - "pubName": "The European Physical Journal C", - "publisher": "Springer Berlin Heidelberg", - "issueNum": "7", - "volumeNum": "83", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "epub", - "issnString": "1434-6052" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1140/epjc/s10052-023-11699-1" - } - ], - "publisherIDs": [ - { - "attribute": "publisher-id", - "Identifier": "s10052-023-11699-1" - }, - { - "attribute": "manuscript", - "Identifier": "11699" - } - ], - "pagination": { - "electronicID": "681" + "abstract": { + "textEnglish": "The flavour-tagging algorithms developed by the ATLAS Collaboration and used to analyse its dataset of s = 13 \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$\\sqrt{s} = 13$$\\end{document} TeV pp collisions from Run 2 of the Large Hadron Collider are presented. These new tagging algorithms are based on recurrent and deep neural networks, and their performance is evaluated in simulated collision events. These developments yield considerable improvements over previous jet-flavour identification strategies. At the 77% b-jet identification efficiency operating point, light-jet (charm-jet) rejection factors of 170 (5) are achieved in a sample of simulated Standard Model t t \u00af \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$t\\bar{t}$$\\end{document} events; similarly, at a c-jet identification efficiency of 30%, a light-jet ( b-jet) rejection factor of 70 (9) is obtained." }, "authors": [ { - "name": { - "surname": "Aad", - "given_name": "G." - }, "affiliation": [ { - "affPubRaw": "CPPM, Aix-Marseille Universit\u00e9, CNRS/IN2P3 Marseille France", - "affPubID": "Aff154" + "affPubID": "Aff154", + "affPubRaw": "CPPM, Aix-Marseille Universit\u00e9, CNRS/IN2P3 Marseille France" } ], "attrib": { "orcid": "0000-0002-6665-4934" + }, + "name": { + "given_name": "G.", + "surname": "Aad" } }, { - "name": { - "surname": "Abbott", - "given_name": "B." - }, "affiliation": [ { - "affPubRaw": "Homer L. Dodge Department of Physics and Astronomy University of Oklahoma Norman OK USA", - "affPubID": "Aff173" + "affPubID": "Aff173", + "affPubRaw": "Homer L. Dodge Department of Physics and Astronomy University of Oklahoma Norman OK USA" } ], "attrib": { "orcid": "0000-0002-5888-2734" + }, + "name": { + "given_name": "B.", + "surname": "Abbott" } }, { - "name": { - "surname": "Abbott", - "given_name": "D. C." - }, "affiliation": [ { - "affPubRaw": "Department of Physics University of Massachusetts Amherst MA USA", - "affPubID": "Aff155" + "affPubID": "Aff155", + "affPubRaw": "Department of Physics University of Massachusetts Amherst MA USA" } ], "attrib": { "orcid": "0000-0002-7248-3203" + }, + "name": { + "given_name": "D. C.", + "surname": "Abbott" } }, { - "name": { - "surname": "Abeling", - "given_name": "K." - }, "affiliation": [ { - "affPubRaw": "II. Physikalisches Institut Georg-August-Universit\u00e4t G\u00f6ttingen G\u00f6ttingen Germany", - "affPubID": "Aff85" + "affPubID": "Aff85", + "affPubRaw": "II. Physikalisches Institut Georg-August-Universit\u00e4t G\u00f6ttingen G\u00f6ttingen Germany" } ], "attrib": { "orcid": "0000-0002-1002-1652" + }, + "name": { + "given_name": "K.", + "surname": "Abeling" } }, { - "name": { - "surname": "Abidi", - "given_name": "S. H." - }, "affiliation": [ { - "affPubRaw": "Physics Department Brookhaven National Laboratory Upton NY USA", - "affPubID": "Aff46" + "affPubID": "Aff46", + "affPubRaw": "Physics Department Brookhaven National Laboratory Upton NY USA" } ], "attrib": { "orcid": "0000-0002-8496-9294" + }, + "name": { + "given_name": "S. H.", + "surname": "Abidi" } }, { - "name": { - "surname": "Aboulhorma", - "given_name": "A." - }, "affiliation": [ { - "affPubRaw": "Facult\u00e9 des sciences Universit\u00e9 Mohammed V Rabat Morocco", - "affPubID": "Aff62" + "affPubID": "Aff62", + "affPubRaw": "Facult\u00e9 des sciences Universit\u00e9 Mohammed V Rabat Morocco" } ], "attrib": { "orcid": "0000-0002-9987-2292" + }, + "name": { + "given_name": "A.", + "surname": "Aboulhorma" } }, { - "name": { - "surname": "Abramowicz", - "given_name": "H." - }, "affiliation": [ { - "affPubRaw": "Raymond and Beverly Sackler School of Physics and Astronomy Tel Aviv University Tel Aviv Israel", - "affPubID": "Aff217" + "affPubID": "Aff217", + "affPubRaw": "Raymond and Beverly Sackler School of Physics and Astronomy Tel Aviv University Tel Aviv Israel" } ], "attrib": { "orcid": "0000-0001-5329-6640" + }, + "name": { + "given_name": "H.", + "surname": "Abramowicz" } }, { - "name": { - "surname": "Abreu", - "given_name": "H." - }, "affiliation": [ { - "affPubRaw": "Department of Physics, Technion Israel Institute of Technology Haifa Israel", - "affPubID": "Aff216" + "affPubID": "Aff216", + "affPubRaw": "Department of Physics, Technion Israel Institute of Technology Haifa Israel" } ], "attrib": { "orcid": "0000-0002-1599-2896" + }, + "name": { + "given_name": "H.", + "surname": "Abreu" } }, { - "name": { - "surname": "Abulaiti", - "given_name": "Y." - }, "affiliation": [ { - "affPubRaw": "Department of Physics New York University New York NY USA", - "affPubID": "Aff170" + "affPubID": "Aff170", + "affPubRaw": "Department of Physics New York University New York NY USA" } ], "attrib": { "orcid": "0000-0003-0403-3697" + }, + "name": { + "given_name": "Y.", + "surname": "Abulaiti" } }, { - "name": { - "surname": "Abusleme Hoffman", - "given_name": "A. 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L.", + "surname": "Zhu" } }, { - "name": { - "surname": "Zhu", - "given_name": "H." - }, "affiliation": [ { - "affPubRaw": "Institute of High Energy Physics Chinese Academy of Sciences Beijing China", - "affPubID": "Aff15" + "affPubID": "Aff15", + "affPubRaw": "Institute of High Energy Physics Chinese Academy of Sciences Beijing China" } ], "attrib": { "orcid": "0000-0001-8066-7048" + }, + "name": { + "given_name": "H.", + "surname": "Zhu" } }, { - "name": { - "surname": "Zhu", - "given_name": "J." - }, "affiliation": [ { - "affPubRaw": "Department of Physics University of Michigan Ann Arbor MI USA", - "affPubID": "Aff158" + "affPubID": "Aff158", + "affPubRaw": "Department of Physics University of Michigan Ann Arbor MI USA" } ], "attrib": { "orcid": "0000-0002-5278-2855" + }, + "name": { + "given_name": "J.", + "surname": "Zhu" } }, { - "name": { - "surname": "Zhu", - "given_name": "Y." - }, "affiliation": [ { - "affPubRaw": "Key Laboratory for Particle Astrophysics and Cosmology (MOE), SKLPPC, School of Physics and Astronomy Shanghai Jiao Tong University Shanghai China", - "affPubID": "Aff95" + "affPubID": "Aff95", + "affPubRaw": "Key Laboratory for Particle Astrophysics and Cosmology (MOE), SKLPPC, School of Physics and Astronomy Shanghai Jiao Tong University Shanghai China" } ], "attrib": { "orcid": "0000-0001-7964-0091" + }, + "name": { + "given_name": "Y.", + "surname": "Zhu" } }, { - "name": { - "surname": "Zhu", - "given_name": "Y." - }, "affiliation": [ { - "affPubRaw": "Department of Modern Physics and State Key Laboratory of Particle Detection and Electronics University of Science and Technology of China Hefei China", - "affPubID": "Aff93" + "affPubID": "Aff93", + "affPubRaw": "Department of Modern Physics and State Key Laboratory of Particle Detection and Electronics University of Science and Technology of China Hefei China" } ], "attrib": { "orcid": "0000-0002-7306-1053" + }, + "name": { + "given_name": "Y.", + "surname": "Zhu" } }, { - "name": { - "surname": "Zhuang", - "given_name": "X." - }, "affiliation": [ { - "affPubRaw": "Institute of High Energy Physics Chinese Academy of Sciences Beijing China", - "affPubID": "Aff15" + "affPubID": "Aff15", + "affPubRaw": "Institute of High Energy Physics Chinese Academy of Sciences Beijing China" } ], "attrib": { "orcid": "0000-0003-0996-3279" + }, + "name": { + "given_name": "X.", + "surname": "Zhuang" } }, { - "name": { - "surname": "Zhukov", - "given_name": "K." - }, "affiliation": [ { - "affPubRaw": "Affiliated with an Institute Covered by a Cooperation Agreement with CERN Geneva Switzerland", - "affPubID": "Aff65" + "affPubID": "Aff65", + "affPubRaw": "Affiliated with an Institute Covered by a Cooperation Agreement with CERN Geneva Switzerland" } ], "attrib": { "orcid": "0000-0003-2468-9634" + }, + "name": { + "given_name": "K.", + "surname": "Zhukov" } }, { - "name": { - "surname": "Zhulanov", - "given_name": "V." - }, "affiliation": [ { - "affPubRaw": "Affiliated with an Institute Covered by a Cooperation Agreement with CERN Geneva Switzerland", - "affPubID": "Aff65" + "affPubID": "Aff65", + "affPubRaw": "Affiliated with an Institute Covered by a Cooperation Agreement with CERN Geneva Switzerland" } ], "attrib": { "orcid": "0000-0002-0306-9199" + }, + "name": { + "given_name": "V.", + "surname": "Zhulanov" } }, { - "name": { - "surname": "Zimine", - "given_name": "N. I." - }, "affiliation": [ { - "affPubRaw": "Affiliated with an International Laboratory Covered by a Cooperation Agreement with CERN Geneva Switzerland", - "affPubID": "Aff66" + "affPubID": "Aff66", + "affPubRaw": "Affiliated with an International Laboratory Covered by a Cooperation Agreement with CERN Geneva Switzerland" } ], "attrib": { "orcid": "0000-0003-0277-4870" + }, + "name": { + "given_name": "N. I.", + "surname": "Zimine" } }, { - "name": { - "surname": "Zinsser", - "given_name": "J." - }, "affiliation": [ { - "affPubRaw": "Physikalisches Institut Ruprecht-Karls-Universit\u00e4t Heidelberg Heidelberg Germany", - "affPubID": "Aff98" + "affPubID": "Aff98", + "affPubRaw": "Physikalisches Institut Ruprecht-Karls-Universit\u00e4t Heidelberg Heidelberg Germany" } ], "attrib": { "orcid": "0000-0002-5117-4671" + }, + "name": { + "given_name": "J.", + "surname": "Zinsser" } }, { - "name": { - "surname": "Ziolkowski", - "given_name": "M." - }, "affiliation": [ { - "affPubRaw": "Department Physik Universit\u00e4t Siegen Siegen Germany", - "affPubID": "Aff205" + "affPubID": "Aff205", + "affPubRaw": "Department Physik Universit\u00e4t Siegen Siegen Germany" } ], "attrib": { "orcid": "0000-0002-2891-8812" + }, + "name": { + "given_name": "M.", + "surname": "Ziolkowski" } }, { - "name": { - "surname": "\u017divkovi\u0107", - "given_name": "L." - }, "affiliation": [ { - "affPubRaw": "Institute of Physics University of Belgrade Belgrade Serbia", - "affPubID": "Aff19" + "affPubID": "Aff19", + "affPubRaw": "Institute of Physics University of Belgrade Belgrade Serbia" } ], "attrib": { "orcid": "0000-0003-4236-8930" + }, + "name": { + "given_name": "L.", + "surname": "\u017divkovi\u0107" } }, { - "name": { - "surname": "Zoccoli", - "given_name": "A." - }, "affiliation": [ { - "affPubRaw": "Dipartimento di Fisica e Astronomia A. Righi Universit\u00e0 di Bologna Bologna Italy", - "affPubID": "Aff32" + "affPubID": "Aff32", + "affPubRaw": "Dipartimento di Fisica e Astronomia A. Righi Universit\u00e0 di Bologna Bologna Italy" }, { - "affPubRaw": "INFN Sezione di Bologna Bologna Italy", - "affPubID": "Aff33" + "affPubID": "Aff33", + "affPubRaw": "INFN Sezione di Bologna Bologna Italy" } ], "attrib": { "orcid": "0000-0002-0993-6185" + }, + "name": { + "given_name": "A.", + "surname": "Zoccoli" } }, { - "name": { - "surname": "Zoch", - "given_name": "K." - }, "affiliation": [ { - "affPubRaw": "D\u00e9partement de Physique Nucl\u00e9aire et Corpusculaire Universit\u00e9 de Gen\u00e8ve Geneva Switzerland", - "affPubID": "Aff86" + "affPubID": "Aff86", + "affPubRaw": "D\u00e9partement de Physique Nucl\u00e9aire et Corpusculaire Universit\u00e9 de Gen\u00e8ve Geneva Switzerland" } ], "attrib": { "orcid": "0000-0003-2138-6187" + }, + "name": { + "given_name": "K.", + "surname": "Zoch" } }, { - "name": { - "surname": "Zorbas", - "given_name": "T. G." - }, "affiliation": [ { - "affPubRaw": "Department of Physics and Astronomy University of Sheffield Sheffield UK", - "affPubID": "Aff203" + "affPubID": "Aff203", + "affPubRaw": "Department of Physics and Astronomy University of Sheffield Sheffield UK" } ], "attrib": { "orcid": "0000-0003-2073-4901" + }, + "name": { + "given_name": "T. G.", + "surname": "Zorbas" } }, { - "name": { - "surname": "Zormpa", - "given_name": "O." - }, "affiliation": [ { - "affPubRaw": "National Centre for Scientific Research \u201cDemokritos\u201d Agia Paraskevi Greece", - "affPubID": "Aff75" + "affPubID": "Aff75", + "affPubRaw": "National Centre for Scientific Research \u201cDemokritos\u201d Agia Paraskevi Greece" } ], "attrib": { "orcid": "0000-0003-3177-903X" + }, + "name": { + "given_name": "O.", + "surname": "Zormpa" } }, { - "name": { - "surname": "Zou", - "given_name": "W." - }, "affiliation": [ { - "affPubRaw": "Nevis Laboratory Columbia University Irvington NY USA", - "affPubID": "Aff69" + "affPubID": "Aff69", + "affPubRaw": "Nevis Laboratory Columbia University Irvington NY USA" } ], "attrib": { "orcid": "0000-0002-0779-8815" + }, + "name": { + "given_name": "W.", + "surname": "Zou" } }, { - "name": { - "surname": "Zwalinski", - "given_name": "L." - }, "affiliation": [ { - "affPubRaw": "CERN Geneva Switzerland", - "affPubID": "Aff64" + "affPubID": "Aff64", + "affPubRaw": "CERN Geneva Switzerland" } ], "attrib": { "orcid": "0000-0002-9397-2313" + }, + "name": { + "given_name": "L.", + "surname": "Zwalinski" } }, { - "name": { - "collab": "ATLAS Collaboration" - }, "attrib": { "collab": true + }, + "name": { + "collab": "ATLAS Collaboration" } } ], - "title": { - "textEnglish": "ATLAS flavour-tagging algorithms for the LHC Run 2 pp collision dataset" + "copyright": { + "statement": "\u00a9 The Author(s) 2023", + "status": true }, - "abstract": { - "textEnglish": "The flavour-tagging algorithms developed by the ATLAS Collaboration and used to analyse its dataset of s = 13 \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$\\sqrt{s} = 13$$\\end{document} TeV pp collisions from Run 2 of the Large Hadron Collider are presented. These new tagging algorithms are based on recurrent and deep neural networks, and their performance is evaluated in simulated collision events. These developments yield considerable improvements over previous jet-flavour identification strategies. At the 77% b-jet identification efficiency operating point, light-jet (charm-jet) rejection factors of 170 (5) are achieved in a sample of simulated Standard Model t t \u00af \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$t\\bar{t}$$\\end{document} events; similarly, at a c-jet identification efficiency of 30%, a light-jet ( b-jet) rejection factor of 70 (9) is obtained." + "editorialHistory": { + "acceptedDate": "2023-01-27", + "receivedDates": [ + "2022-11-30" + ] + }, + "openAccess": { + "license": "\nOpen Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article\u2019s Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article\u2019s Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit\n\t\t\t\t\t\thttp://creativecommons.org/licenses/by/4.0/.\n\t\t\t\t\t", + "licenseURL": "http://creativecommons.org/licenses/by/4.0/", + "open": true + }, + "pagination": { + "electronicID": "681" + }, + "persistentIDs": [ + { + "DOI": "10.1140/epjc/s10052-023-11699-1" + } + ], + "pubDate": { + "electrDate": "2023-07-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "1434-6052", + "pubtype": "epub" + } + ], + "issueNum": "7", + "pubName": "The European Physical Journal C", + "pubYear": "2023", + "publisher": "Springer Berlin Heidelberg", + "volumeNum": "83" + }, + "publisherIDs": [ + { + "Identifier": "s10052-023-11699-1", + "attribute": "publisher-id" + }, + { + "Identifier": "11699", + "attribute": "manuscript" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " ATLAS Collaboration, The ATLAS experiment at the CERN large hadron collider. JINST \t\t\t\t\t\t3, S08003 (2008). \t\t\t\t\t\thttps://doi.org/10.1088/1748-0221/3/08/S08003 ", @@ -44968,13 +44974,7 @@ " ATLAS Collaboration, Calibration of light-flavour b-jet mistagging rates using ATLAS proton\u2013proton collision data at \t\t\t\t\t\t s = 13 TeV \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$\\sqrt{s} = 13~\\text{ TeV }$$\\end{document} . ATLAS-CONF-2018-006 (2018). \t\t\t\t\t\thttps://cds.cern.ch/record/2314418 ", " ATLAS Collaboration, ATLAS computing acknowledgements. ATL-SOFT-PUB-2021-003 (2021). \t\t\t\t\t\thttps://cds.cern.ch/record/2776662 " ], - "copyright": { - "status": true, - "statement": "\u00a9 The Author(s) 2023" - }, - "openAccess": { - "open": true, - "license": "\nOpen Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article\u2019s Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article\u2019s Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit\n\t\t\t\t\t\thttp://creativecommons.org/licenses/by/4.0/.\n\t\t\t\t\t", - "licenseURL": "http://creativecommons.org/licenses/by/4.0/" + "title": { + "textEnglish": "ATLAS flavour-tagging algorithms for the LHC Run 2 pp collision dataset" } } diff --git a/tests/stubdata/output/jats_springer_EPJC_s10052-023-11733-2.json b/tests/stubdata/output/jats_springer_EPJC_s10052-023-11733-2.json index 423d633..3c59cde 100644 --- a/tests/stubdata/output/jats_springer_EPJC_s10052-023-11733-2.json +++ b/tests/stubdata/output/jats_springer_EPJC_s10052-023-11733-2.json @@ -1,15195 +1,15201 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2022-06-30" - ], - "acceptedDate": "2023-06-20" - }, - "pubDate": { - "electrDate": "2023-07-00" - }, - "publication": { - "pubName": "The European Physical Journal C", - "publisher": "Springer Berlin Heidelberg", - "issueNum": "7", - "volumeNum": "83", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "epub", - "issnString": "1434-6052" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1140/epjc/s10052-023-11733-2" - } - ], - "publisherIDs": [ - { - "attribute": "publisher-id", - "Identifier": "s10052-023-11733-2" - }, - { - "attribute": "manuscript", - "Identifier": "11733" - } - ], - "pagination": { - "electronicID": "618" + "abstract": { + "textEnglish": "The Pandora Software Development Kit and algorithm libraries provide pattern-recognition logic essential to the reconstruction of particle interactions in liquid argon time projection chamber detectors. Pandora is the primary event reconstruction software used at ProtoDUNE-SP, a prototype for the Deep Underground Neutrino Experiment far detector. ProtoDUNE-SP, located at CERN, is exposed to a charged-particle test beam. This paper gives an overview of the Pandora reconstruction algorithms and how they have been tailored for use at ProtoDUNE-SP. In complex events with numerous cosmic-ray and beam background particles, the simulated reconstruction and identification efficiency for triggered test-beam particles is above 80% for the majority of particle type and beam momentum combinations. Specifically, simulated 1 GeV/ c charged pions and protons are correctly reconstructed and identified with efficiencies of 86.1 \u00b1 0.6 \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$\\pm 0.6$$\\end{document} % and 84.1 \u00b1 0.6 \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$\\pm 0.6$$\\end{document} %, respectively. The efficiencies measured for test-beam data are shown to be within 5% of those predicted by the simulation." }, "authors": [ { - "name": { - "surname": "Abud", - "given_name": "A. Abed" - }, "affiliation": [ { - "affPubRaw": "CERN, The European Organization for Nuclear Research 1211 Meyrin Switzerland", - "affPubID": "Aff35" + "affPubID": "Aff35", + "affPubRaw": "CERN, The European Organization for Nuclear Research 1211 Meyrin Switzerland" }, { - "affPubRaw": "University of Liverpool L69 7ZE Liverpool UK", - "affPubID": "Aff130" + "affPubID": "Aff130", + "affPubRaw": "University of Liverpool L69 7ZE Liverpool UK" } - ] + ], + "name": { + "given_name": "A. Abed", + "surname": "Abud" + } }, { - "name": { - "surname": "Abi", - "given_name": "B." - }, "affiliation": [ { - "affPubRaw": "University of Oxford OX1 3RH Oxford UK", - "affPubID": "Aff158" + "affPubID": "Aff158", + "affPubRaw": "University of Oxford OX1 3RH Oxford UK" } - ] + ], + "name": { + "given_name": "B.", + "surname": "Abi" + } }, { - "name": { - "surname": "Acciarri", - "given_name": "R." - }, "affiliation": [ { - "affPubRaw": "Fermi National Accelerator Laboratory 60510 Batavia IL USA", - "affPubID": "Aff67" + "affPubID": "Aff67", + "affPubRaw": "Fermi National Accelerator Laboratory 60510 Batavia IL USA" } - ] + ], + "name": { + "given_name": "R.", + "surname": "Acciarri" + } }, { - "name": { - "surname": "Acero", - "given_name": "M. A." - }, "affiliation": [ { - "affPubRaw": "Universidad del Atl\u00e1ntico Barranquilla Atl\u00e1ntico Colombia", - "affPubID": "Aff11" + "affPubID": "Aff11", + "affPubRaw": "Universidad del Atl\u00e1ntico Barranquilla Atl\u00e1ntico Colombia" } - ] + ], + "name": { + "given_name": "M. A.", + "surname": "Acero" + } }, { - "name": { - "surname": "Adames", - "given_name": "M. R." - }, "affiliation": [ { - "affPubRaw": "Universidade Tecnol\u00f3gica Federal do Paran\u00e1 Curitiba Brazil", - "affPubID": "Aff195" + "affPubID": "Aff195", + "affPubRaw": "Universidade Tecnol\u00f3gica Federal do Paran\u00e1 Curitiba Brazil" } - ] + ], + "name": { + "given_name": "M. R.", + "surname": "Adames" + } }, { - "name": { - "surname": "Adamov", - "given_name": "G." - }, "affiliation": [ { - "affPubRaw": "Georgian Technical University Tbilisi Georgia", - "affPubID": "Aff72" + "affPubID": "Aff72", + "affPubRaw": "Georgian Technical University Tbilisi Georgia" } - ] + ], + "name": { + "given_name": "G.", + "surname": "Adamov" + } }, { - "name": { - "surname": "Adamowski", - "given_name": "M." - }, "affiliation": [ { - "affPubRaw": "Fermi National Accelerator Laboratory 60510 Batavia IL USA", - "affPubID": "Aff67" + "affPubID": "Aff67", + "affPubRaw": "Fermi National Accelerator Laboratory 60510 Batavia IL USA" } - ] + ], + "name": { + "given_name": "M.", + "surname": "Adamowski" + } }, { - "name": { - "surname": "Adams", - "given_name": "D." - }, "affiliation": [ { - "affPubRaw": "Brookhaven National Laboratory 11973 Upton NY USA", - "affPubID": "Aff20" + "affPubID": "Aff20", + "affPubRaw": "Brookhaven National Laboratory 11973 Upton NY USA" } - ] + ], + "name": { + "given_name": "D.", + "surname": "Adams" + } }, { - "name": { - "surname": "Adinolfi", - "given_name": "M." - }, "affiliation": [ { - "affPubRaw": "University of Bristol BS8 1TL Bristol UK", - "affPubID": "Aff19" + "affPubID": "Aff19", + "affPubRaw": "University of Bristol BS8 1TL Bristol UK" } - ] + ], + "name": { + "given_name": "M.", + "surname": "Adinolfi" + } }, { - "name": { - "surname": "Adriano", - "given_name": "C." - }, "affiliation": [ { - "affPubRaw": "Universidade Estadual de Campinas 13083-970 Campinas SP Brazil", - "affPubID": "Aff30" + "affPubID": "Aff30", + "affPubRaw": "Universidade Estadual de Campinas 13083-970 Campinas SP Brazil" } - ] + ], + "name": { + "given_name": "C.", + "surname": "Adriano" + } }, { - "name": { - "surname": "Aduszkiewicz", - "given_name": "A." - }, "affiliation": [ { - "affPubRaw": "University of Houston 77204 Houston TX USA", - "affPubID": "Aff81" + "affPubID": "Aff81", + "affPubRaw": "University of Houston 77204 Houston TX USA" } - ] + ], + "name": { + "given_name": "A.", + "surname": "Aduszkiewicz" + } }, { - "name": { - "surname": "Aguilar", - "given_name": "J." - }, "affiliation": [ { - "affPubRaw": "Lawrence Berkeley National Laboratory 94720 Berkeley CA USA", - "affPubID": "Aff128" + "affPubID": "Aff128", + "affPubRaw": "Lawrence Berkeley National Laboratory 94720 Berkeley CA USA" } - ] + ], + "name": { + "given_name": "J.", + "surname": "Aguilar" + } }, { - "name": { - "surname": "Ahmad", - "given_name": "Z." - }, "affiliation": [ { - "affPubRaw": "Variable Energy Cyclotron Centre 700 064 Kolkata West Bengal India", - "affPubID": "Aff206" + "affPubID": "Aff206", + "affPubRaw": "Variable Energy Cyclotron Centre 700 064 Kolkata West Bengal India" } - ] + ], + "name": { + "given_name": "Z.", + "surname": "Ahmad" + } }, { - "name": { - "surname": "Ahmed", - "given_name": "J." - }, "affiliation": [ { - "affPubRaw": "University of Warwick CV4 7AL Coventry UK", - "affPubID": "Aff209" + "affPubID": "Aff209", + "affPubRaw": "University of Warwick CV4 7AL Coventry UK" } - ] + ], + "name": { + "given_name": "J.", + "surname": "Ahmed" + } }, { - "name": { - "surname": "Aimard", - "given_name": "B." - }, "affiliation": [ { - "affPubRaw": "Laboratoire d\u2019Annecy de Physique des Particules, Univ. 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D." - }, "affiliation": [ { - "affPubRaw": "University of Colorado Boulder 80309 Boulder CO USA", - "affPubID": "Aff43" + "affPubID": "Aff43", + "affPubRaw": "University of Colorado Boulder 80309 Boulder CO USA" } - ] + ], + "name": { + "given_name": "E. D.", + "surname": "Zimmerman" + } }, { - "name": { - "surname": "Zucchelli", - "given_name": "S." - }, "affiliation": [ { - "affPubRaw": "Universit\u00e0 del Bologna 40127 Bologna Italy", - "affPubID": "Aff17" + "affPubID": "Aff17", + "affPubRaw": "Universit\u00e0 del Bologna 40127 Bologna Italy" }, { - "affPubRaw": "Istituto Nazionale di Fisica Nucleare Sezione di Bologna 40127 Bologna BO Italy", - "affPubID": "Aff92" + "affPubID": "Aff92", + "affPubRaw": "Istituto Nazionale di Fisica Nucleare Sezione di Bologna 40127 Bologna BO Italy" } - ] + ], + "name": { + "given_name": "S.", + "surname": "Zucchelli" + } }, { - "name": { - "surname": "Zuklin", - "given_name": "J." - }, "affiliation": [ { - "affPubRaw": "Institute of Physics Czech Academy of Sciences 182 00 Prague 8 Czech Republic", - "affPubID": "Aff48" + "affPubID": "Aff48", + "affPubRaw": "Institute of Physics Czech Academy of Sciences 182 00 Prague 8 Czech Republic" } - ] + ], + "name": { + "given_name": "J.", + "surname": "Zuklin" + } }, { - "name": { - "surname": "Zutshi", - "given_name": "V." - }, "affiliation": [ { - "affPubRaw": "Northern Illinois University 60115 DeKalb IL USA", - "affPubID": "Aff152" + "affPubID": "Aff152", + "affPubRaw": "Northern Illinois University 60115 DeKalb IL USA" } - ] + ], + "name": { + "given_name": "V.", + "surname": "Zutshi" + } }, { - "name": { - "surname": "Zwaska", - "given_name": "R." - }, "affiliation": [ { - "affPubRaw": "Fermi National Accelerator Laboratory 60510 Batavia IL USA", - "affPubID": "Aff67" + "affPubID": "Aff67", + "affPubRaw": "Fermi National Accelerator Laboratory 60510 Batavia IL USA" } - ] + ], + "name": { + "given_name": "R.", + "surname": "Zwaska" + } }, { - "name": { - "collab": "DUNE Collaboration" - }, "attrib": { "collab": true + }, + "name": { + "collab": "DUNE Collaboration" } } ], - "title": { - "textEnglish": "Reconstruction of interactions in the ProtoDUNE-SP detector with Pandora" + "copyright": { + "statement": "\u00a9 The Author(s) 2023", + "status": true }, - "abstract": { - "textEnglish": "The Pandora Software Development Kit and algorithm libraries provide pattern-recognition logic essential to the reconstruction of particle interactions in liquid argon time projection chamber detectors. Pandora is the primary event reconstruction software used at ProtoDUNE-SP, a prototype for the Deep Underground Neutrino Experiment far detector. ProtoDUNE-SP, located at CERN, is exposed to a charged-particle test beam. This paper gives an overview of the Pandora reconstruction algorithms and how they have been tailored for use at ProtoDUNE-SP. In complex events with numerous cosmic-ray and beam background particles, the simulated reconstruction and identification efficiency for triggered test-beam particles is above 80% for the majority of particle type and beam momentum combinations. Specifically, simulated 1 GeV/ c charged pions and protons are correctly reconstructed and identified with efficiencies of 86.1 \u00b1 0.6 \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$\\pm 0.6$$\\end{document} % and 84.1 \u00b1 0.6 \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$\\pm 0.6$$\\end{document} %, respectively. The efficiencies measured for test-beam data are shown to be within 5% of those predicted by the simulation." + "editorialHistory": { + "acceptedDate": "2023-06-20", + "receivedDates": [ + "2022-06-30" + ] + }, + "openAccess": { + "license": "\nOpen Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article\u2019s Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article\u2019s Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit\n\t\t\t\t\t\thttp://creativecommons.org/licenses/by/4.0/.\n\t\t\t\t\t", + "licenseURL": "http://creativecommons.org/licenses/by/4.0/", + "open": true + }, + "pagination": { + "electronicID": "618" + }, + "persistentIDs": [ + { + "DOI": "10.1140/epjc/s10052-023-11733-2" + } + ], + "pubDate": { + "electrDate": "2023-07-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "1434-6052", + "pubtype": "epub" + } + ], + "issueNum": "7", + "pubName": "The European Physical Journal C", + "pubYear": "2023", + "publisher": "Springer Berlin Heidelberg", + "volumeNum": "83" + }, + "publisherIDs": [ + { + "Identifier": "s10052-023-11733-2", + "attribute": "publisher-id" + }, + { + "Identifier": "11733", + "attribute": "manuscript" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " A. Abed Abud et al. Design, construction and operation of the ProtoDUNE-SP Liquid Argon TPC. JINST \t\t\t\t\t\t17(01), P01005 (2022). \t\t\t\t\t\thttps://doi.org/10.1088/1748-0221/17/01/p01005 ", @@ -15220,13 +15226,7 @@ " E. Gramellini, \t\t\t\t\t\tMeasurement of the Negative Pion and Positive Kaon Total Hadronic Cross Sections on Argon at the LArIAT Experiment Ph.D. thesis, Yale U. (2018) \t\t\t\t\t ", " E. Gramellini et al. Measurement of the ( \t\t\t\t\t\t \u03c0 - \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$\\pi ^-$$\\end{document} , Ar) total hadronic cross section at the LArIAT experiment (2021). \t\t\t\t\t\tarXiv:2108.00040 [physics.ins-det] \t\t\t\t\t " ], - "copyright": { - "status": true, - "statement": "\u00a9 The Author(s) 2023" - }, - "openAccess": { - "open": true, - "license": "\nOpen Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article\u2019s Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article\u2019s Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit\n\t\t\t\t\t\thttp://creativecommons.org/licenses/by/4.0/.\n\t\t\t\t\t", - "licenseURL": "http://creativecommons.org/licenses/by/4.0/" + "title": { + "textEnglish": "Reconstruction of interactions in the ProtoDUNE-SP detector with Pandora" } } diff --git a/tests/stubdata/output/jats_springer_NatCo_s41467-023-40272-3.json b/tests/stubdata/output/jats_springer_NatCo_s41467-023-40272-3.json index d231dfe..78ac24e 100644 --- a/tests/stubdata/output/jats_springer_NatCo_s41467-023-40272-3.json +++ b/tests/stubdata/output/jats_springer_NatCo_s41467-023-40272-3.json @@ -1,664 +1,675 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2023-02-17" - ], - "acceptedDate": "2023-07-20" - }, - "pubDate": { - "electrDate": "2023-12-00" - }, - "publication": { - "pubName": "Nature Communications", - "publisher": "Nature Publishing Group UK", - "issueNum": "1", - "volumeNum": "14", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "epub", - "issnString": "2041-1723" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1038/s41467-023-40272-3" - } - ], - "publisherIDs": [ - { - "attribute": "publisher-id", - "Identifier": "s41467-023-40272-3" - }, - { - "attribute": "manuscript", - "Identifier": "40272" - } - ], - "pagination": { - "electronicID": "4551" + "abstract": { + "textEnglish": "A Gamma Variant RBD-based aluminum hydroxide adjuvanted vaccine called ARVAC CG was selected for a first in human clinical trial. Healthy male and female participants (18-55 years old) with a complete COVID-19-primary vaccine scheme were assigned to receive two intramuscular doses of either a low-dose or a high-dose of ARVAC CG. The primary endpoint was safety. The secondary objective was humoral immunogenicity. Cellular immune responses were studied as an exploratory objective. The trial was prospectively registered in PRIISA.BA (Registration Code 6564) and ANMAT and retrospectively registered in ClinicalTrials.gov (NCT05656508). Samples from participants of a surveillance strategy implemented by the Ministry of Health of the Province of Buenos Aires that were boosted with BNT162b2 were also analyzed to compare with the booster effect of ARVAC CG. ARVAC CG exhibits a satisfactory safety profile, a robust and broad booster response of neutralizing antibodies against the Ancestral strain of SARS-CoV-2 and the Gamma, Delta, Omicron BA.1 and Omicron BA.5 variants of concern and a booster effect on T cell immunity in individuals previously immunized with different COVID-19 vaccine platforms." }, "authors": [ { - "name": { - "surname": "Pasquevich", - "given_name": "Karina A." - }, "affiliation": [ { - "affPubRaw": "Instituto de Investigaciones Biotecnol\u00f3gicas Universidad Nacional de San Mart\u00edn (UNSAM) \u2013 Consejo Nacional de Investigaciones Cient\u00edficas y T\u00e9cnicas (CONICET) San Mart\u00edn (1650) Buenos Aires Argentina", - "affPubID": "Aff1" + "affPubID": "Aff1", + "affPubRaw": "Instituto de Investigaciones Biotecnol\u00f3gicas Universidad Nacional de San Mart\u00edn (UNSAM) \u2013 Consejo Nacional de Investigaciones Cient\u00edficas y T\u00e9cnicas (CONICET) San Mart\u00edn (1650) Buenos Aires Argentina" }, { - "affPubRaw": "Escuela de Bio y Nanotecnolog\u00edas (EByN) Universidad Nacional de San Mart\u00edn San Mart\u00edn (1650) Buenos Aires Argentina", - "affPubID": "Aff2" + "affPubID": "Aff2", + "affPubRaw": "Escuela de Bio y Nanotecnolog\u00edas (EByN) Universidad Nacional de San Mart\u00edn San Mart\u00edn (1650) Buenos Aires Argentina" } ], "attrib": { "email": "kpasquevich@iib.unsam.edu.ar", "orcid": "0000-0003-4448-0977" + }, + "name": { + "given_name": "Karina A.", + "surname": "Pasquevich" } }, { - "name": { - "surname": "Coria", - "given_name": "Lorena M." - }, "affiliation": [ { - "affPubRaw": "Instituto de Investigaciones Biotecnol\u00f3gicas Universidad Nacional de San Mart\u00edn (UNSAM) \u2013 Consejo Nacional de Investigaciones Cient\u00edficas y T\u00e9cnicas (CONICET) San Mart\u00edn (1650) Buenos Aires Argentina", - "affPubID": "Aff1" + "affPubID": "Aff1", + "affPubRaw": "Instituto de Investigaciones Biotecnol\u00f3gicas Universidad Nacional de San Mart\u00edn (UNSAM) \u2013 Consejo Nacional de Investigaciones Cient\u00edficas y T\u00e9cnicas (CONICET) San Mart\u00edn (1650) Buenos Aires Argentina" }, { - 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"name": { - "surname": "Kaufmann", - "given_name": "Ingrid G.", - "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium" - }, "affiliation": [ { - "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina" } ], "attrib": { "collab": true + }, + "name": { + "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium", + "given_name": "Ingrid G.", + "surname": "Kaufmann" } }, { - "name": { - "surname": "Di Mar\u00eda", - "given_name": "Adri\u00e1n", - "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium" - }, "affiliation": [ { - "affPubRaw": "Instituto de Investigaciones Biotecnol\u00f3gicas Universidad Nacional de San Mart\u00edn (UNSAM) \u2013 Consejo Nacional de Investigaciones Cient\u00edficas y T\u00e9cnicas (CONICET) San Mart\u00edn (1650) Buenos Aires Argentina", - 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"name": { - "surname": "Moreno", - "given_name": "Agust\u00edn", - "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium" - }, "affiliation": [ { - "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina" } ], "attrib": { "collab": true + }, + "name": { + "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium", + "given_name": "Agust\u00edn", + "surname": "Moreno" } }, { - "name": { - "surname": "Cervellini", - "given_name": "Susana", - "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium" - }, "affiliation": [ { - "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina", - 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"name": { - "surname": "Ali", - "given_name": "Esteban", - "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium" - }, "affiliation": [ { - "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina" } ], "attrib": { "collab": true + }, + "name": { + "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium", + "given_name": "Esteban", + "surname": "Ali" } }, { - "name": { - "surname": "Albarrac\u00edn", - "given_name": "Romina", - "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium" - }, "affiliation": [ { - "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina", - 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"name": { - "surname": "Toneguzzo", - "given_name": "Fernando", - "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium" - }, "affiliation": [ { - "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina" } ], "attrib": { "collab": true + }, + "name": { + "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium", + "given_name": "Fernando", + "surname": "Toneguzzo" } }, { - "name": { - "surname": "Sasso", - "given_name": "Guillermina", - "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium" - }, "affiliation": [ { - "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina", - 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"name": { - "surname": "Cardoso", - "given_name": "Regina", - "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium" - }, "affiliation": [ { - "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina" } ], "attrib": { "collab": true + }, + "name": { + "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium", + "given_name": "Regina", + "surname": "Cardoso" } }, { - "name": { - "surname": "Chajet", - "given_name": "Alejandro", - "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium" - }, "affiliation": [ { - "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina" } ], "attrib": { "collab": true + }, + "name": { + "collab": "Laboratorio Pablo Cassar\u00e1 R&D and CMC for ARVAC CG consortium", + "given_name": "Alejandro", + "surname": "Chajet" } }, { - "name": { - "surname": "Feleder", - "given_name": "Ethel" - }, "affiliation": [ { - "affPubRaw": "FP CLINICAL PHARMA Ciudad Aut\u00f3noma de Buenos Aires Buenos Aires Argentina", - "affPubID": "Aff6" + "affPubID": "Aff6", + "affPubRaw": "FP CLINICAL PHARMA Ciudad Aut\u00f3noma de Buenos Aires Buenos Aires Argentina" } - ] + ], + "name": { + "given_name": "Ethel", + "surname": "Feleder" + } }, { - "name": { - "surname": "Halabe", - "given_name": "Karina" - }, "affiliation": [ { - "affPubRaw": "FP CLINICAL PHARMA Ciudad Aut\u00f3noma de Buenos Aires Buenos Aires Argentina", - "affPubID": "Aff6" + "affPubID": "Aff6", + "affPubRaw": "FP CLINICAL PHARMA Ciudad Aut\u00f3noma de Buenos Aires Buenos Aires Argentina" } - ] + ], + "name": { + "given_name": "Karina", + "surname": "Halabe" + } }, { - "name": { - "surname": "Perez Lera", - "given_name": "Pablo E." - }, "affiliation": [ { - "affPubRaw": "FP CLINICAL PHARMA Ciudad Aut\u00f3noma de Buenos Aires Buenos Aires Argentina", - "affPubID": "Aff6" + "affPubID": "Aff6", + "affPubRaw": "FP CLINICAL PHARMA Ciudad Aut\u00f3noma de Buenos Aires Buenos Aires Argentina" } - ] + ], + "name": { + "given_name": "Pablo E.", + "surname": "Perez Lera" + } }, { - "name": { - "surname": "de Oca", - "given_name": "Federico Montes" - }, "affiliation": [ { - "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina" } - ] + ], + "name": { + "given_name": "Federico Montes", + "surname": "de Oca" + } }, { - "name": { - "surname": "Vega", - "given_name": "Julio C." - }, "affiliation": [ { - "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina" } - ] + ], + "name": { + "given_name": "Julio C.", + "surname": "Vega" + } }, { - "name": { - "surname": "Lombardo", - "given_name": "M\u00f3nica" - }, "affiliation": [ { - "affPubRaw": "Nobeltri Ciudad Aut\u00f3noma de Buenos Aires Argentina", - "affPubID": "Aff8" + "affPubID": "Aff8", + "affPubRaw": "Nobeltri Ciudad Aut\u00f3noma de Buenos Aires Argentina" } - ] + ], + "name": { + "given_name": "M\u00f3nica", + "surname": "Lombardo" + } }, { - "name": { - "surname": "Yerino", - "given_name": "Gustavo A." - }, "affiliation": [ { - "affPubRaw": "FP CLINICAL PHARMA Ciudad Aut\u00f3noma de Buenos Aires Buenos Aires Argentina", - "affPubID": "Aff6" + "affPubID": "Aff6", + "affPubRaw": "FP CLINICAL PHARMA Ciudad Aut\u00f3noma de Buenos Aires Buenos Aires Argentina" } - ] + ], + "name": { + "given_name": "Gustavo A.", + "surname": "Yerino" + } }, { - "name": { - "surname": "Fl\u00f3", - "given_name": "Juan" - }, "affiliation": [ { - "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Laboratorio Pablo Cassar\u00e1 \u2013 Unidad de I + D de Biof\u00e1rmacos Saladillo 2452 C1440FFX Ciudad Aut\u00f3noma de Buenos Aires Argentina" } ], "attrib": { "orcid": "0000-0002-0051-7435" + }, + "name": { + "given_name": "Juan", + "surname": "Fl\u00f3" } }, { - "name": { - "surname": "Cassataro", - "given_name": "Juliana" - }, "affiliation": [ { - "affPubRaw": "Instituto de Investigaciones Biotecnol\u00f3gicas Universidad Nacional de San Mart\u00edn (UNSAM) \u2013 Consejo Nacional de Investigaciones Cient\u00edficas y T\u00e9cnicas (CONICET) San Mart\u00edn (1650) Buenos Aires Argentina", - "affPubID": "Aff1" + "affPubID": "Aff1", + "affPubRaw": "Instituto de Investigaciones Biotecnol\u00f3gicas Universidad Nacional de San Mart\u00edn (UNSAM) \u2013 Consejo Nacional de Investigaciones Cient\u00edficas y T\u00e9cnicas (CONICET) San Mart\u00edn (1650) Buenos Aires Argentina" }, { - "affPubRaw": "Escuela de Bio y Nanotecnolog\u00edas (EByN) Universidad Nacional de San Mart\u00edn San Mart\u00edn (1650) Buenos Aires Argentina", - "affPubID": "Aff2" + "affPubID": "Aff2", + "affPubRaw": "Escuela de Bio y Nanotecnolog\u00edas (EByN) Universidad Nacional de San Mart\u00edn San Mart\u00edn (1650) Buenos Aires Argentina" } ], "attrib": { "email": "jucassataro@iib.unsam.edu.ar", "orcid": "0000-0002-7122-869X" + }, + "name": { + "given_name": "Juliana", + "surname": "Cassataro" } } ], - "title": { - "textEnglish": "Safety and immunogenicity of a SARS-CoV-2 Gamma variant RBD-based protein adjuvanted vaccine used as booster in healthy adults" + "copyright": { + "statement": "\u00a9 The Author(s) 2023", + "status": true }, - "abstract": { - "textEnglish": "A Gamma Variant RBD-based aluminum hydroxide adjuvanted vaccine called ARVAC CG was selected for a first in human clinical trial. Healthy male and female participants (18-55 years old) with a complete COVID-19-primary vaccine scheme were assigned to receive two intramuscular doses of either a low-dose or a high-dose of ARVAC CG. The primary endpoint was safety. The secondary objective was humoral immunogenicity. Cellular immune responses were studied as an exploratory objective. The trial was prospectively registered in PRIISA.BA (Registration Code 6564) and ANMAT and retrospectively registered in ClinicalTrials.gov (NCT05656508). Samples from participants of a surveillance strategy implemented by the Ministry of Health of the Province of Buenos Aires that were boosted with BNT162b2 were also analyzed to compare with the booster effect of ARVAC CG. ARVAC CG exhibits a satisfactory safety profile, a robust and broad booster response of neutralizing antibodies against the Ancestral strain of SARS-CoV-2 and the Gamma, Delta, Omicron BA.1 and Omicron BA.5 variants of concern and a booster effect on T cell immunity in individuals previously immunized with different COVID-19 vaccine platforms." + "editorialHistory": { + "acceptedDate": "2023-07-20", + "receivedDates": [ + "2023-02-17" + ] + }, + "funding": [ + { + "agencyname": "Laboratorio Pablo Cassara" + } + ], + "openAccess": { + "license": "\nOpen Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article\u2019s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article\u2019s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit\n\t\t\t\t\t\thttp://creativecommons.org/licenses/by/4.0/.\n\t\t\t\t\t", + "licenseURL": "http://creativecommons.org/licenses/by/4.0/", + "open": true + }, + "pagination": { + "electronicID": "4551" + }, + "persistentIDs": [ + { + "DOI": "10.1038/s41467-023-40272-3" + } + ], + "pubDate": { + "electrDate": "2023-12-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "2041-1723", + "pubtype": "epub" + } + ], + "issueNum": "1", + "pubName": "Nature Communications", + "pubYear": "2023", + "publisher": "Nature Publishing Group UK", + "volumeNum": "14" + }, + "publisherIDs": [ + { + "Identifier": "s41467-023-40272-3", + "attribute": "publisher-id" + }, + { + "Identifier": "40272", + "attribute": "manuscript" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " Chi W-Y COVID-19 vaccine update: vaccine effectiveness, SARS-CoV-2 variants, boosters, adverse effects, and immune correlates of protection J. Biomed. Sci. 2022 29 10.1186/s12929-022-00853-8 36243868 9569411 ", @@ -693,18 +704,7 @@ " Varese A Omicron Breakthrough Infection After Heterologous Prime-Boost Vaccination Induces a Vigorous Antibody Response J. Infect. Dis. 2022 226 1717 1720 1:CAS:528:DC%2BB3sXptFart7w%3D 10.1093/infdis/jiac250 35723970 ", " World_Health_Organization. WHO manual for the establishment of national and other secondary standards for antibodies against infectious agents focusing on SARSCoV2. (World Health Organization, 2022). " ], - "copyright": { - "status": true, - "statement": "\u00a9 The Author(s) 2023" - }, - "openAccess": { - "open": true, - "license": "\nOpen Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article\u2019s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article\u2019s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit\n\t\t\t\t\t\thttp://creativecommons.org/licenses/by/4.0/.\n\t\t\t\t\t", - "licenseURL": "http://creativecommons.org/licenses/by/4.0/" - }, - "funding": [ - { - "agencyname": "Laboratorio Pablo Cassara" - } - ] + "title": { + "textEnglish": "Safety and immunogenicity of a SARS-CoV-2 Gamma variant RBD-based protein adjuvanted vaccine used as booster in healthy adults" + } } diff --git a/tests/stubdata/output/jats_springer_Natur_s41598-023-38673-x.json b/tests/stubdata/output/jats_springer_Natur_s41598-023-38673-x.json index 22a6ef4..5812da0 100644 --- a/tests/stubdata/output/jats_springer_Natur_s41598-023-38673-x.json +++ b/tests/stubdata/output/jats_springer_Natur_s41598-023-38673-x.json @@ -1,881 +1,896 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" - }, - "editorialHistory": { - "receivedDates": [ - "2022-09-09" - ], - "acceptedDate": "2023-07-12" - }, - "pubDate": { - "electrDate": "2023-12-00" - }, - "publication": { - "pubName": "Scientific Reports", - "publisher": "Nature Publishing Group UK", - "issueNum": "1", - "volumeNum": "13", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "epub", - "issnString": "2045-2322" - } - ] - }, - "persistentIDs": [ - { - "DOI": "10.1038/s41598-023-38673-x" - } - ], - "publisherIDs": [ - { - "attribute": "publisher-id", - "Identifier": "s41598-023-38673-x" - }, - { - "attribute": "manuscript", - "Identifier": "38673" - } - ], - "pagination": { - "electronicID": "11732" + "abstract": { + "textEnglish": "A growing body of literature suggests the important role of the thalamus in cognition and neurodegenerative diseases. This study aims to elucidate whether the preoperative thalamic volume is associated with preoperative cognitive impairment (preCI) and whether it is predictive for postoperative cognitive dysfunction at 3 months (POCD). We enrolled 301 patients aged 65 or older and without signs of dementia who were undergoing elective surgery. Magnetic resonance imaging was conducted prior to surgery. Freesurfer (version 5.3.) was used to automatically segment the thalamus volume. A neuropsychological test battery was administered before surgery and at a 3 month follow-up. It included the computerized tests Paired Associate Learning (PAL), Verbal Recognition Memory (VRM), Spatial Span Length (SSP), Simple Reaction Time (SRT), the pen-and-paper Trail-Making-Test (TMT) and the manual Grooved Pegboard Test (GPT). Using a reliable change index, preCI and POCD were defined as total Z-score > 1.96 (sum score over all tests) and/or Z-scores > 1.96 in \u2265 2 individual cognitive test parameters. For statistical analyses, multivariable logistic regression models were applied. Age, sex and intracranial volume were covariates in the models. Of 301 patients who received a presurgical neuropsychological testing and MRI, 34 (11.3%) had preCI. 89 patients (29.5%) were lost to follow-up. The remaining 212 patients received a follow-up cognitive test after 3 months, of whom 25 (8.3%) presented with POCD. Independently of age, sex and intracranial volume, neither preCI (OR per cm 3 increment 0.81 [95% CI 0.60\u20131.07] p = 0.14) nor POCD (OR 1.02 per cm 3 increment [95% CI 0.75\u20131.40] p = 0.87) were statistically significantly associated with patients\u2019 preoperative thalamus volume. In this cohort we could not show an association of presurgical thalamus volume with preCI or POCD.\nClinical Trial Number: NCT02265263 ( https://clinicaltrials.gov/ct2/show/results/NCT02265263) ." }, "authors": [ { - "name": { - "surname": "Fislage", - "given_name": "Marinus" - }, "affiliation": [ { - "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK), Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany", - "affPubID": "Aff1" + "affPubID": "Aff1", + "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK), Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany" } ], "attrib": { "email": "marinus.fislage@charite.de", "orcid": "0000-0001-9102-1373" + }, + "name": { + "given_name": "Marinus", + "surname": "Fislage" } }, { - "name": { - "surname": "Feinkohl", - "given_name": "Insa" - }, "affiliation": [ { - "affPubRaw": "Faculty of Health/School of Medicine Witten/Herdecke University Witten Germany", - "affPubID": "Aff2" + "affPubID": "Aff2", + "affPubRaw": "Faculty of Health/School of Medicine Witten/Herdecke University Witten Germany" }, { - "affPubRaw": "Molecular Epidemiology Research Group Max-Delbrueck-Center for Molecular Medicine in the Helmholtz Association (MDC) Berlin Germany", - "affPubID": "Aff3" + "affPubID": "Aff3", + "affPubRaw": "Molecular Epidemiology Research Group Max-Delbrueck-Center for Molecular Medicine in the Helmholtz Association (MDC) Berlin Germany" } ], "attrib": { "orcid": "0000-0002-0307-1862" + }, + "name": { + "given_name": "Insa", + "surname": "Feinkohl" } }, { - "name": { - "surname": "Borchers", - "given_name": "Friedrich" - }, "affiliation": [ { - "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK), Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany", - "affPubID": "Aff1" + "affPubID": "Aff1", + "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK), Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany" } ], "attrib": { "orcid": "0000-0001-7290-2271" + }, + "name": { + "given_name": "Friedrich", + "surname": "Borchers" } }, { - "name": { - "surname": "Pischon", - "given_name": "Tobias" - }, "affiliation": [ { - "affPubRaw": "Molecular Epidemiology Research Group Max-Delbrueck-Center for Molecular Medicine in the Helmholtz Association (MDC) Berlin Germany", - "affPubID": "Aff3" + "affPubID": "Aff3", + "affPubRaw": "Molecular Epidemiology Research Group Max-Delbrueck-Center for Molecular Medicine in the Helmholtz Association (MDC) Berlin Germany" }, { - "affPubRaw": "Biobank Technology Platform Max-Delbrueck-Center for Molecular Medicine in the Helmholtz Association (MDC) Berlin Germany", - "affPubID": "Aff4" + "affPubID": "Aff4", + "affPubRaw": "Biobank Technology Platform Max-Delbrueck-Center for Molecular Medicine in the Helmholtz Association (MDC) Berlin Germany" }, { - "affPubRaw": "Core Facility Biobank Berlin Institute of Health at Charit\u00e9 - Universit\u00e4tsmedizin Berlin Berlin Germany", - "affPubID": "Aff5" + "affPubID": "Aff5", + "affPubRaw": "Core Facility Biobank Berlin Institute of Health at Charit\u00e9 - Universit\u00e4tsmedizin Berlin Berlin Germany" } ], "attrib": { "orcid": "0000-0003-1568-767X" + }, + "name": { + "given_name": "Tobias", + "surname": "Pischon" } }, { - "name": { - "surname": "Spies", - "given_name": "Claudia D." - }, "affiliation": [ { - "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK), Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany", - "affPubID": "Aff1" + "affPubID": "Aff1", + "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK), Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany" } ], "attrib": { "orcid": "0000-0002-1062-0495" + }, + "name": { + "given_name": "Claudia D.", + "surname": "Spies" } }, { - "name": { - "surname": "Winterer", - "given_name": "Georg" - }, "affiliation": [ { - "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK), Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany", - "affPubID": "Aff1" + "affPubID": "Aff1", + "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK), Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany" }, { - "affPubRaw": "Pharmaimage Biomarker Solutions GmbH Berlin Germany", - "affPubID": "Aff6" + "affPubID": "Aff6", + "affPubRaw": "Pharmaimage Biomarker Solutions GmbH Berlin Germany" } ], "attrib": { "orcid": "0000-0002-3610-5029" + }, + "name": { + "given_name": "Georg", + "surname": "Winterer" } }, { - "name": { - "surname": "Zacharias", - "given_name": "Norman" - 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"name": { - "surname": "Wolf", - "given_name": "Alissa", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Alissa", + "surname": "Wolf" } }, { - "name": { - "surname": "M\u00fcller", - "given_name": "Anika", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Anika", + "surname": "M\u00fcller" } }, { - "name": { - "surname": "Hadzidiakos", - "given_name": "Daniel", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Daniel", + "surname": "Hadzidiakos" } }, { - "name": { - "surname": "Y\u00fcrek", - "given_name": "Fatima", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Fatima", + "surname": "Y\u00fcrek" } }, { - "name": { - "surname": "Lachmann", - "given_name": "Gunnar", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Gunnar", + "surname": "Lachmann" } }, { - "name": { - "surname": "Ofosu", - "given_name": "Kwaku", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Kwaku", + "surname": "Ofosu" } }, { - "name": { - "surname": "Heinrich", - "given_name": "Maria", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Maria", + "surname": "Heinrich" } }, { - "name": { - "surname": "M\u00f6rgeli", - "given_name": "Rudolf", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany", - "affPubID": "Aff7" + "affPubID": "Aff7", + "affPubRaw": "Department of Anesthesiology and Operative Intensive Care Medicine (CCM, CVK) Charit\u00e9\u2013Universit\u00e4tsmedizin Berlin, Corporate Member of Freie Universit\u00e4t Berlin and Humboldt-Universit\u00e4t zu Berlin Berlin Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Rudolf", + "surname": "M\u00f6rgeli" } }, { - "name": { - "surname": "Gallinat", - "given_name": "J\u00fcrgen", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University Medical Center Hamburg Hamburg Germany", - "affPubID": "Aff8" + "affPubID": "Aff8", + "affPubRaw": "University Medical Center Hamburg Hamburg Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "J\u00fcrgen", + "surname": "Gallinat" } }, { - "name": { - "surname": "K\u00fchn", - "given_name": "Simone", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University Medical Center Hamburg Hamburg Germany", - "affPubID": "Aff8" + "affPubID": "Aff8", + "affPubRaw": "University Medical Center Hamburg Hamburg Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Simone", + "surname": "K\u00fchn" } }, { - "name": { - "surname": "Slooter", - "given_name": "Arjen", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University Medical Center Utrecht Utrecht The Netherlands", - "affPubID": "Aff9" + "affPubID": "Aff9", + "affPubRaw": "University Medical Center Utrecht Utrecht The Netherlands" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Arjen", + "surname": "Slooter" } }, { - "name": { - "surname": "van Dellen", - "given_name": "Edwin", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University Medical Center Utrecht Utrecht The Netherlands", - "affPubID": "Aff9" + "affPubID": "Aff9", + "affPubRaw": "University Medical Center Utrecht Utrecht The Netherlands" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Edwin", + "surname": "van Dellen" } }, { - "name": { - "surname": "Kant", - "given_name": "Ilse", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University Medical Center Utrecht Utrecht The Netherlands", - "affPubID": "Aff9" + "affPubID": "Aff9", + "affPubRaw": "University Medical Center Utrecht Utrecht The Netherlands" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Ilse", + "surname": "Kant" } }, { - "name": { - "surname": "de Bresser", - "given_name": "Jeroen", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University Medical Center Utrecht Utrecht The Netherlands", - "affPubID": "Aff9" + "affPubID": "Aff9", + "affPubRaw": "University Medical Center Utrecht Utrecht The Netherlands" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Jeroen", + "surname": "de Bresser" } }, { - "name": { - "surname": "Hendrikse", - "given_name": "Jeroen", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University Medical Center Utrecht Utrecht The Netherlands", - "affPubID": "Aff9" + "affPubID": "Aff9", + "affPubRaw": "University Medical Center Utrecht Utrecht The Netherlands" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Jeroen", + "surname": "Hendrikse" } }, { - "name": { - "surname": "van Montfort", - "given_name": "Simone", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University Medical Center Utrecht Utrecht The Netherlands", - "affPubID": "Aff9" + "affPubID": "Aff9", + "affPubRaw": "University Medical Center Utrecht Utrecht The Netherlands" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Simone", + "surname": "van Montfort" } }, { - "name": { - "surname": "Menon", - "given_name": "David", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University of Cambridge Cambridge UK", - "affPubID": "Aff10" + "affPubID": "Aff10", + "affPubRaw": "University of Cambridge Cambridge UK" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "David", + "surname": "Menon" } }, { - "name": { - "surname": "Stamatakis", - "given_name": "Emmanuel", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University of Cambridge Cambridge UK", - "affPubID": "Aff10" + "affPubID": "Aff10", + "affPubRaw": "University of Cambridge Cambridge UK" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Emmanuel", + "surname": "Stamatakis" } }, { - "name": { - "surname": "Preller", - "given_name": "Jacobus", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University of Cambridge Cambridge UK", - "affPubID": "Aff10" + "affPubID": "Aff10", + "affPubRaw": "University of Cambridge Cambridge UK" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Jacobus", + "surname": "Preller" } }, { - "name": { - "surname": "Moreno-L\u00f3pez", - "given_name": "Laura", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University of Cambridge Cambridge UK", - "affPubID": "Aff10" + "affPubID": "Aff10", + "affPubRaw": "University of Cambridge Cambridge UK" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Laura", + "surname": "Moreno-L\u00f3pez" } }, { - "name": { - "surname": "Winzeck", - "given_name": "Stefan", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University of Cambridge Cambridge UK", - "affPubID": "Aff10" + "affPubID": "Aff10", + "affPubRaw": "University of Cambridge Cambridge UK" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Stefan", + "surname": "Winzeck" } }, { - "name": { - "surname": "Melillo", - "given_name": "Daniela", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "National Research Council Napoli Naples Italy", - "affPubID": "Aff11" + "affPubID": "Aff11", + "affPubRaw": "National Research Council Napoli Naples Italy" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Daniela", + "surname": "Melillo" } }, { - "name": { - "surname": "Boraschi", - "given_name": "Diana", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "National Research Council Napoli Naples Italy", - "affPubID": "Aff11" + "affPubID": "Aff11", + "affPubRaw": "National Research Council Napoli Naples Italy" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Diana", + "surname": "Boraschi" } }, { - "name": { - "surname": "Camera", - "given_name": "Giacomo Della", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "National Research Council Napoli Naples Italy", - "affPubID": "Aff11" + "affPubID": "Aff11", + "affPubRaw": "National Research Council Napoli Naples Italy" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Giacomo Della", + "surname": "Camera" } }, { - "name": { - "surname": "Italiani", - "given_name": "Paola", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "National Research Council Napoli Naples Italy", - "affPubID": "Aff11" + "affPubID": "Aff11", + "affPubRaw": "National Research Council Napoli Naples Italy" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Paola", + "surname": "Italiani" } }, { - "name": { - "surname": "Schneider", - "given_name": "Reinhard", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University of Luxembourg Esch-sur-Alzette Luxembourg", - "affPubID": "Aff12" + "affPubID": "Aff12", + "affPubRaw": "University of Luxembourg Esch-sur-Alzette Luxembourg" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Reinhard", + "surname": "Schneider" } }, { - "name": { - "surname": "Krause", - "given_name": "Roland", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "University of Luxembourg Esch-sur-Alzette Luxembourg", - "affPubID": "Aff12" + "affPubID": "Aff12", + "affPubRaw": "University of Luxembourg Esch-sur-Alzette Luxembourg" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Roland", + "surname": "Krause" } }, { - "name": { - "surname": "Heidtke", - "given_name": "Karsten", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "ATLAS Biolabs GmBH Berlin Germany", - "affPubID": "Aff13" + "affPubID": "Aff13", + "affPubRaw": "ATLAS Biolabs GmBH Berlin Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Karsten", + "surname": "Heidtke" } }, { - "name": { - "surname": "N\u00fcrnberg", - "given_name": "Peter", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "ATLAS Biolabs GmBH Berlin Germany", - "affPubID": "Aff13" + "affPubID": "Aff13", + "affPubRaw": "ATLAS Biolabs GmBH Berlin Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Peter", + "surname": "N\u00fcrnberg" } }, { - "name": { - "surname": "Helmschrodt", - "given_name": "Anja", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Immundiagnostik AG Bensheim Germany", - "affPubID": "Aff14" + "affPubID": "Aff14", + "affPubRaw": "Immundiagnostik AG Bensheim Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Anja", + "surname": "Helmschrodt" } }, { - "name": { - "surname": "B\u00f6cher", - "given_name": "Axel", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Immundiagnostik AG Bensheim Germany", - "affPubID": "Aff14" + "affPubID": "Aff14", + "affPubRaw": "Immundiagnostik AG Bensheim Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Axel", + "surname": "B\u00f6cher" } }, { - "name": { - "surname": "Hafen", - "given_name": "Bettina", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Immundiagnostik AG Bensheim Germany", - "affPubID": "Aff14" + "affPubID": "Aff14", + "affPubRaw": "Immundiagnostik AG Bensheim Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Bettina", + "surname": "Hafen" } }, { - "name": { - "surname": "Armbruster", - "given_name": "Franz Paul", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Immundiagnostik AG Bensheim Germany", - "affPubID": "Aff14" + "affPubID": "Aff14", + "affPubRaw": "Immundiagnostik AG Bensheim Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Franz Paul", + "surname": "Armbruster" } }, { - "name": { - "surname": "Diehl", - "given_name": "Ina", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Immundiagnostik AG Bensheim Germany", - "affPubID": "Aff14" + "affPubID": "Aff14", + "affPubRaw": "Immundiagnostik AG Bensheim Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Ina", + "surname": "Diehl" } }, { - "name": { - "surname": "Ruppert", - "given_name": "Jana", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Immundiagnostik AG Bensheim Germany", - "affPubID": "Aff14" + "affPubID": "Aff14", + "affPubRaw": "Immundiagnostik AG Bensheim Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Jana", + "surname": "Ruppert" } }, { - "name": { - "surname": "Hartmann", - "given_name": "Katarina", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Immundiagnostik AG Bensheim Germany", - "affPubID": "Aff14" + "affPubID": "Aff14", + "affPubRaw": "Immundiagnostik AG Bensheim Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Katarina", + "surname": "Hartmann" } }, { - "name": { - "surname": "Kronabel", - "given_name": "Marion", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Immundiagnostik AG Bensheim Germany", - "affPubID": "Aff14" + "affPubID": "Aff14", + "affPubRaw": "Immundiagnostik AG Bensheim Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Marion", + "surname": "Kronabel" } }, { - "name": { - "surname": "Weyer", - "given_name": "Marius", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Immundiagnostik AG Bensheim Germany", - "affPubID": "Aff14" + "affPubID": "Aff14", + "affPubRaw": "Immundiagnostik AG Bensheim Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Marius", + "surname": "Weyer" } }, { - "name": { - "surname": "Dschietzig", - "given_name": "Thomas Bernd", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Immundiagnostik AG Bensheim Germany", - "affPubID": "Aff14" + "affPubID": "Aff14", + "affPubRaw": "Immundiagnostik AG Bensheim Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Thomas Bernd", + "surname": "Dschietzig" } }, { - "name": { - "surname": "Pietzsch", - "given_name": "Malte", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Cellogic GmbH Berlin Germany", - "affPubID": "Aff15" + "affPubID": "Aff15", + "affPubRaw": "Cellogic GmbH Berlin Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Malte", + "surname": "Pietzsch" } }, { - "name": { - "surname": "Weber", - "given_name": "Simon", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Cellogic GmbH Berlin Germany", - "affPubID": "Aff15" + "affPubID": "Aff15", + "affPubRaw": "Cellogic GmbH Berlin Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Simon", + "surname": "Weber" } }, { - "name": { - "surname": "Ittermann", - "given_name": "Bernd", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Physikalisch-Technische Bundesanstalt Berlin Germany", - "affPubID": "Aff16" + "affPubID": "Aff16", + "affPubRaw": "Physikalisch-Technische Bundesanstalt Berlin Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Bernd", + "surname": "Ittermann" } }, { - "name": { - "surname": "Fillmer", - "given_name": "Ariane", - "collab": "BioCog Consortium" - }, "affiliation": [ { - "affPubRaw": "Physikalisch-Technische Bundesanstalt Berlin Germany", - "affPubID": "Aff16" + "affPubID": "Aff16", + "affPubRaw": "Physikalisch-Technische Bundesanstalt Berlin Germany" } ], "attrib": { "collab": true + }, + "name": { + "collab": "BioCog Consortium", + "given_name": "Ariane", + "surname": "Fillmer" } } ], - "title": { - "textEnglish": "Preoperative thalamus volume is not associated with preoperative cognitive impairment (preCI) or postoperative cognitive dysfunction (POCD)" + "copyright": { + "statement": "\u00a9 The Author(s) 2023. corrected publication 2023", + "status": true }, - "abstract": { - "textEnglish": "A growing body of literature suggests the important role of the thalamus in cognition and neurodegenerative diseases. This study aims to elucidate whether the preoperative thalamic volume is associated with preoperative cognitive impairment (preCI) and whether it is predictive for postoperative cognitive dysfunction at 3 months (POCD). We enrolled 301 patients aged 65 or older and without signs of dementia who were undergoing elective surgery. Magnetic resonance imaging was conducted prior to surgery. Freesurfer (version 5.3.) was used to automatically segment the thalamus volume. A neuropsychological test battery was administered before surgery and at a 3 month follow-up. It included the computerized tests Paired Associate Learning (PAL), Verbal Recognition Memory (VRM), Spatial Span Length (SSP), Simple Reaction Time (SRT), the pen-and-paper Trail-Making-Test (TMT) and the manual Grooved Pegboard Test (GPT). Using a reliable change index, preCI and POCD were defined as total Z-score > 1.96 (sum score over all tests) and/or Z-scores > 1.96 in \u2265 2 individual cognitive test parameters. For statistical analyses, multivariable logistic regression models were applied. Age, sex and intracranial volume were covariates in the models. Of 301 patients who received a presurgical neuropsychological testing and MRI, 34 (11.3%) had preCI. 89 patients (29.5%) were lost to follow-up. The remaining 212 patients received a follow-up cognitive test after 3 months, of whom 25 (8.3%) presented with POCD. Independently of age, sex and intracranial volume, neither preCI (OR per cm 3 increment 0.81 [95% CI 0.60\u20131.07] p = 0.14) nor POCD (OR 1.02 per cm 3 increment [95% CI 0.75\u20131.40] p = 0.87) were statistically significantly associated with patients\u2019 preoperative thalamus volume. In this cohort we could not show an association of presurgical thalamus volume with preCI or POCD.\nClinical Trial Number: NCT02265263 ( https://clinicaltrials.gov/ct2/show/results/NCT02265263) ." + "editorialHistory": { + "acceptedDate": "2023-07-12", + "receivedDates": [ + "2022-09-09" + ] + }, + "funding": [ + { + "agencyname": "European Community's FP7", + "awardnumber": "602461" + }, + { + "agencyname": "Charit\u00e9 - Universit\u00e4tsmedizin Berlin (3093)" + } + ], + "openAccess": { + "license": "\nOpen Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit\n\t\t\t\t\t\thttp://creativecommons.org/licenses/by/4.0/.\n\t\t\t\t\t", + "licenseURL": "http://creativecommons.org/licenses/by/4.0/", + "open": true + }, + "pagination": { + "electronicID": "11732" + }, + "persistentIDs": [ + { + "DOI": "10.1038/s41598-023-38673-x" + } + ], + "pubDate": { + "electrDate": "2023-12-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "2045-2322", + "pubtype": "epub" + } + ], + "issueNum": "1", + "pubName": "Scientific Reports", + "pubYear": "2023", + "publisher": "Nature Publishing Group UK", + "volumeNum": "13" + }, + "publisherIDs": [ + { + "Identifier": "s41598-023-38673-x", + "attribute": "publisher-id" + }, + { + "Identifier": "38673", + "attribute": "manuscript" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " Androsova G Krause R Winterer G Schneider R Biomarkers of postoperative delirium and cognitive dysfunction Front. Aging Neurosci. 2015 7 112 26106326 4460425 ", @@ -922,22 +937,7 @@ " Berger M Terrando N Smith SK Browndyke JN Newman MF Mathew JP Neurocognitive function after cardiac surgery: From phenotypes to mechanisms Anesthesiology 2018 129 829 851 29621031 ", " Dieleman N Koek HL Hendrikse J Short-term mechanisms influencing volumetric brain dynamics Neuroimage Clin. 2017 16 507 513 28971004 5609861 " ], - "copyright": { - "status": true, - "statement": "\u00a9 The Author(s) 2023. corrected publication 2023" - }, - "openAccess": { - "open": true, - "license": "\nOpen Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit\n\t\t\t\t\t\thttp://creativecommons.org/licenses/by/4.0/.\n\t\t\t\t\t", - "licenseURL": "http://creativecommons.org/licenses/by/4.0/" - }, - "funding": [ - { - "agencyname": "European Community's FP7", - "awardnumber": "602461" - }, - { - "agencyname": "Charit\u00e9 - Universit\u00e4tsmedizin Berlin (3093)" - } - ] + "title": { + "textEnglish": "Preoperative thalamus volume is not associated with preoperative cognitive impairment (preCI) or postoperative cognitive dysfunction (POCD)" + } } diff --git a/tests/stubdata/output/jats_springer_ZaMP_s00033-023-02064-z.json b/tests/stubdata/output/jats_springer_ZaMP_s00033-023-02064-z.json index 578beac..6847da0 100644 --- a/tests/stubdata/output/jats_springer_ZaMP_s00033-023-02064-z.json +++ b/tests/stubdata/output/jats_springer_ZaMP_s00033-023-02064-z.json @@ -1,111 +1,156 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "JATS", - "loadLocation": "", - "recordOrigin": "" + "abstract": { + "textEnglish": "This paper is concerned with the time-asymptotic stability of a nonlinear wave for the outflow problem of the isentropic compressible Navier\u2013Stokes\u2013Korteweg equations in the half space. Under some suitable assumptions on the spatial-asymptotic states and boundary data, the time-asymptotic profile is a nonlinear wave which is the superposition of a stationary solution and a rarefaction wave. Employing the L 2 \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$L^{2}$$\\end{document} -energy method and the decay (in both time and space variables) estimates of each component of the nonlinear wave, we prove that this nonlinear wave is time asymptotically stable under a small initial perturbation." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "Aff1", + "affPubRaw": "School of Sciences Nantong University 226019 Nantong People\u2019s Republic of China" + } + ], + "name": { + "given_name": "Yeping", + "surname": "Li" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff1", + "affPubRaw": "School of Sciences Nantong University 226019 Nantong People\u2019s Republic of China" + } + ], + "name": { + "given_name": "Rui", + "surname": "Xu" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff2", + "affPubRaw": "School of Mathematical Sciences Anhui University 230601 Hefei People\u2019s Republic of China" + }, + { + "affPubID": "Aff3", + "affPubRaw": "Centre of Pure Mathematics, School of Mathematical Sciences Anhui University 230601 Hefei People\u2019s Republic of China" + } + ], + "attrib": { + "email": "chenzzandu@163.com", + "orcid": "0000-0002-4062-3267" + }, + "name": { + "given_name": "Zhengzheng", + "surname": "Chen" + } + } + ], + "copyright": { + "statement": "\u00a9 The Author(s), under exclusive licence to Springer Nature Switzerland AG 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.", + "status": true }, "editorialHistory": { + "acceptedDate": "2023-07-04", "receivedDates": [ "2021-05-14" ], "revisedDates": [ "2023-07-04" - ], - "acceptedDate": "2023-07-04" - }, - "pubDate": { - "electrDate": "2023-07-19", - "printDate": "2023-08-00" - }, - "publication": { - "pubName": "Zeitschrift f\u00fcr angewandte Mathematik und Physik", - "publisher": "Springer International Publishing", - "issueNum": "4", - "volumeNum": "74", - "pubYear": "2023", - "ISSN": [ - { - "pubtype": "ppub", - "issnString": "0044-2275" - }, - { - "pubtype": "epub", - "issnString": "1420-9039" - } ] }, - "persistentIDs": [ + "funding": [ { - "DOI": "10.1007/s00033-023-02064-z" + "agencyid": { + "idschema": "doi", + "idvalue": "http://dx.doi.org/10.13039/501100001809" + }, + "agencyname": "National Natural Science Foundation of China", + "awardnumber": "12171258" + }, + { + "agencyname": "Support Program for Outstanding Young Talents in Universities of Anhui Province", + "awardnumber": "gxyqZD2022007" } ], - "publisherIDs": [ + "keywords": [ + { + "keyString": "Compressible Navier\u2013Stokes\u2013Korteweg equations", + "keySystem": "misc" + }, + { + "keyString": "Asymptotic stability", + "keySystem": "misc" + }, { - "attribute": "publisher-id", - "Identifier": "s00033-023-02064-z" + "keyString": "Rarefaction wave", + "keySystem": "misc" + }, + { + "keyString": "Stationary solution", + "keySystem": "misc" }, { - "attribute": "manuscript", - "Identifier": "2064" + "keyString": "Energy method", + "keySystem": "misc" + }, + { + "keyString": "76W05", + "keySystem": "misc" + }, + { + "keyString": "35B40", + "keySystem": "misc" } ], "pagination": { "electronicID": "167" }, - "authors": [ + "persistentIDs": [ { - "name": { - "surname": "Li", - "given_name": "Yeping" + "DOI": "10.1007/s00033-023-02064-z" + } + ], + "pubDate": { + "electrDate": "2023-07-19", + "printDate": "2023-08-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "0044-2275", + "pubtype": "ppub" }, - "affiliation": [ - { - "affPubRaw": "School of Sciences Nantong University 226019 Nantong People\u2019s Republic of China", - "affPubID": "Aff1" - } - ] - }, + { + "issnString": "1420-9039", + "pubtype": "epub" + } + ], + "issueNum": "4", + "pubName": "Zeitschrift f\u00fcr angewandte Mathematik und Physik", + "pubYear": "2023", + "publisher": "Springer International Publishing", + "volumeNum": "74" + }, + "publisherIDs": [ { - "name": { - "surname": "Xu", - "given_name": "Rui" - }, - "affiliation": [ - { - "affPubRaw": "School of Sciences Nantong University 226019 Nantong People\u2019s Republic of China", - "affPubID": "Aff1" - } - ] + "Identifier": "s00033-023-02064-z", + "attribute": "publisher-id" }, { - "name": { - "surname": "Chen", - "given_name": "Zhengzheng" - }, - "affiliation": [ - { - "affPubRaw": "School of Mathematical Sciences Anhui University 230601 Hefei People\u2019s Republic of China", - "affPubID": "Aff2" - }, - { - "affPubRaw": "Centre of Pure Mathematics, School of Mathematical Sciences Anhui University 230601 Hefei People\u2019s Republic of China", - "affPubID": "Aff3" - } - ], - "attrib": { - "email": "chenzzandu@163.com", - "orcid": "0000-0002-4062-3267" - } + "Identifier": "2064", + "attribute": "manuscript" } ], - "title": { - "textEnglish": "Asymptotic stability of a nonlinear wave for the compressible Navier\u2013Stokes\u2013Korteweg equations in the half space" - }, - "abstract": { - "textEnglish": "This paper is concerned with the time-asymptotic stability of a nonlinear wave for the outflow problem of the isentropic compressible Navier\u2013Stokes\u2013Korteweg equations in the half space. Under some suitable assumptions on the spatial-asymptotic states and boundary data, the time-asymptotic profile is a nonlinear wave which is the superposition of a stationary solution and a rarefaction wave. Employing the L 2 \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$L^{2}$$\\end{document} -energy method and the decay (in both time and space variables) estimates of each component of the nonlinear wave, we prove that this nonlinear wave is time asymptotically stable under a small initial perturbation." + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ " Bresch D Desjardins B Lin C-K On some compressible fluid models: Korteweg, lubrication and shallow water systems Commun. Partial Differ. Equ. 2003 28 843 868 1978317 1106.76436 10.1081/PDE-120020499 ", @@ -162,52 +207,7 @@ " Wang Y-J Tan Z Optimal decay rates for the compressible fluid models of Korteweg type J. Math. Anal. Appl. 2011 379 256 271 2776470 1211.35228 10.1016/j.jmaa.2011.01.006 ", " Wang W-J Wang W-K Decay rate of the compressible Navier-Stokes-Korteweg equations with potential force Dis. Contin. Dyn. Syst. 2015 35 513 536 3286970 1304.35576 10.3934/dcds.2015.35.513 " ], - "keywords": [ - { - "keyString": "Compressible Navier\u2013Stokes\u2013Korteweg equations", - "keySystem": "misc" - }, - { - "keyString": "Asymptotic stability", - "keySystem": "misc" - }, - { - "keyString": "Rarefaction wave", - "keySystem": "misc" - }, - { - "keyString": "Stationary solution", - "keySystem": "misc" - }, - { - "keyString": "Energy method", - "keySystem": "misc" - }, - { - "keyString": "76W05", - "keySystem": "misc" - }, - { - "keyString": "35B40", - "keySystem": "misc" - } - ], - "copyright": { - "status": true, - "statement": "\u00a9 The Author(s), under exclusive licence to Springer Nature Switzerland AG 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law." - }, - "funding": [ - { - "agencyname": "National Natural Science Foundation of China", - "agencyid": { - "idschema": "doi", - "idvalue": "http://dx.doi.org/10.13039/501100001809" - }, - "awardnumber": "12171258" - }, - { - "agencyname": "Support Program for Outstanding Young Talents in Universities of Anhui Province", - "awardnumber": "gxyqZD2022007" - } - ] + "title": { + "textEnglish": "Asymptotic stability of a nonlinear wave for the compressible Navier\u2013Stokes\u2013Korteweg equations in the half space" + } } diff --git a/tests/stubdata/output/wiley_jgra_12057.json b/tests/stubdata/output/wiley_jgra_12057.json index 5b27a2e..afd1d0b 100644 --- a/tests/stubdata/output/wiley_jgra_12057.json +++ b/tests/stubdata/output/wiley_jgra_12057.json @@ -1,61 +1,132 @@ -{"abstract": {"textEnglish": "The path‐integrated linear growth of electromagnetic ion cyclotron waves in the outer (L ≥ 7) magnetosphere is investigated using a realistic thermal plasma distribution with an additional anisotropic energetic ring current H+ to provide free energy for instability. The results provide a realistic simulation of the recent AMPTE observations. For conditions typical of the dayside magnetosphere, high plasma beta effects reduce the group velocity and significantly increase the spatial growth rates for left‐hand polarized instabilities just below the helium gyrofrequency ΩHe+, and on the unguided mode above Ω>He+ but below the cross over frequency ωcr. Relatively high densities, typical of the afternoon local time sector, favor these low group velocity effects for predominantly field‐aligned waves. Lower densities, typical of those found in the early morning local time sector, increase the group velocity but allow strong convective instabilities at high normalized frequencies well above ΩHe+. These waves are reflected in the magnetosphere and can exist for several equatorial transits without significant damping. They are left‐hand polarized only on the first equatorial crossing and become linearly polarized for the remainder of the ray path. Consequently, these waves should be observed with basically linear polarization at all frequencies and all latitudes in the early morning local time sector. Wave growth below ΩHe+ is severely limited owing to the narrow bandwidth for instability and the small resonant path lengths. In the afternoon sector, where plasma densities can exceed 107 m−3, intense convective amplification is possible both above and below ΩHe+. Waves below ΩHe+ are not subject to reflection when the O+ concentration is small and therefore should be observed with left‐hand polarization near the equator and essentially linear polarization at higher latitudes. Since the He+ concentration is usually large in the afternoon sector, guided mode waves above ΩHe+ reflect to form a background distribution with basically linear polarization. We suggest that the strong left‐hand polarized emissions observed by AMPTE in the afternoon sector near the equator are probably due to strongly growing low group velocity waves at frequencies just below ΩHe+, and on the unguided mode above ΩHe+."}, - "authors": [{"name": {"given_name": "Richard B.", "surname": "Horne"}}, {"name": {"given_name": "Richard M.", "surname": "Thorne"}}], - "copyright": {"statement": "Copyright 1994 by the American Geophysical Union.", "status": true}, - "editorialHistory": {"acceptedDate": "1994-05-12", "receivedDates": ["1993-05-24"]}, - "pagination": {"firstPage": "17259", "lastPage": "17273", "pageCount": "15"}, - "persistentIDs": [{"DOI": "10.1029/94JA01259"}], - "pubDate": {"electrDate": "2012-09-20", "printDate": "1994-09-01"}, - "publication": {"ISSN": [{"issnString": "0148-0227", "pubtype": "print"}, {"issnString": "2156-2202", "pubtype": "electronic"}], "issueNum": "A9", "pubName": "Journal of Geophysical Research: Space Physics", "pubYear": "1994", "volumeNum": "99"}, - "publisherIDs": [{"Identifier": "94JA01259", "attribute": "editorialOffice"}, {"Identifier": "JGRA12057", "attribute": "unit"}], - "recordData": {"createdTime": "", "loadFormat": "OtherXML", "loadLocation": "", "loadType": "fromFile", "parsedTime": "", "recordOrigin": ""}, - "references": ["Anderson, B. J., D. C. Hamilton, Electromagnetic ion cyclotron waves stimulated by modest magnetospheric compressions, J. Geophys. Res., 9811, 369, 1993.", - "Anderson, B. J., K. Takahashi, R. E. Erlandson, L. J. Zanetti, Pc1 pulsations observed by AMPTE/CCE in the Earth's outer magnetosphere, Geophys. Res. Lett., 17, 1853, 1990.", - "Anderson, B. J., R. E. Erlandson, L. J. Zanetti, A statistical study of Pc 1–2 magnetic pulsations in the equatorial magnetosphere, 1, Equatorial occurrence distributions, J. Geophys. Res., 97, 3075, 1992a.", - "Anderson, B. J., R. E. Erlandson, L. J. Zanetti, A statistical study of Pc 1–2 magnetic pulsations in the equatorial magnetosphere, 2, Wave properties, J. Geophys. Res., 97, 3089, 1992b.", - "André, M., Dispersion surfaces, J. Plasma Phys., 33, 1, 1985.", - "Ashour‐ Abdalla, M., C. F. Kennel, Nonconvective and convective electron cyclotron harmonic instabilities, J. Geophys. Res., 83, 1531, 1978.", - "Bossen, M., R. L. McPherron, C. T. Russel, A statistical study of pc 1 magnetic pulsations at synchronous Orbit, J. Geophys. Res., 81, 6083, 1976.", - "Budden, K. G., The Propagation of Radio Waves, Cambridge University Press, New York, 1985.", - "Cornwall, J. M., F. V. Coroniti, R. M. Thorne, Turbulent loss of ring current protons, J. Geophys. Res., 75, 4699, 1970.", - "Cornwall, J. M., F. V. Coroniti, R. M. Thorne, Unified theory of SAR arc formation at the plasmapause, J. Geophys. Res., 76, 4428, 1971.", - "Denton, R. E., M. K. Hudson, I. Roth, Loss‐cone‐driven ion cyclotron waves in the magnetosphere, J. Geophys. Res., 9712, 093, 1992.", - "Fried, B. D., S. D. Conte, The Plasma Dispersion Function, Academic, San Diego, Calif., 1961.", - "Fraser, B. J., W. J. Kemp, D. J. Webster, Ground‐satellite study of a Pc 1 ion cyclotron wave event, J. Geophys. Res., 9411, 855, 1989.", - "Fraser, B. J., R. L. McPherron, Pc 1–2 magnetic pulsation spectra and heavy ion effects at synchronous orbit: ATS 6 results, J. Geophys. Res., 87, 4560, 1982.", - "Gendrin, R., A. Roux, Energization of helium ions by proton induced hydromagnetic waves, J. Geophys. Res., 85, 4577, 1980.", - "Gendrin, R., M. Ashour‐Abdalla, Y. Omura, K. Quest, Linear analysis of ion cyclotron interaction in a multicomponent plasma, J. Geophys. Res., 89, 9119, 1984.", - "Gloeckler, G., B. Wilken, W. Studemann, F. M. Ipavich, D. Hovestadt, D. C. Hamilton, G. Kremser, First composition measurement of the bulk of the storm time ring‐current (1 to 300 keV/e) with AMPTE‐CCE, Geophys. Res. Lett., 12, 325, 1985.", - "Gomberoff, L., R. Neira, Convective growth rate of ion cyclotron waves in a H+‐He+ and H+‐He+‐O+ plasma, J. Geophys. Res., 88, 2170, 1983.", - "Higel, B., L. Wu, Electron density and plasmapause characteristics at 6.6RE, A statistical study of the GEOS 2 relaxation sounder data, J. Geophys. Res., 89, 1583, 1984.", - "Horne, R. B., Path‐integrated growth of electrostatic waves: The generation of terrestrial myriametric radiation, J. Geophys. Res., 94, 8895, 1989.", - "Horne, R. B., R. M. Thorne, Ion cyclotron absorption at the second harmonic of the oxygen gyrofrequency, Geophys. Res. Lett., 17, 2225, 1990.", - "Horne, R. B., R. M. Thorne, On the preferred source location for the convective amplification of ion cyclotron waves, J. Geophys. Res., 98, 9233, 1993.", - "Hu, Y. D., B. J. Fraser, J. V. Olsen, Amplification of electromagnetic ion cyclotron waves along a wave path in the Earth's multi‐component magnetosphere, Geophys. Res., Lett., 17, 1053, 1990.", - "Hu, Y. D., B. J. Fraser, Electromagnetic ion cyclotron wave amplification and source regions in the magnetosphere, J. Geophys. Res., 99, 263, 1994.", - "Inan, U. S., T. F. Bell, The plasmapause as a VLF wave guide, J. Geophys. Res., 19, 2819, 1977.", - "Ishida, I., S. Kokubun, R. L. McPherron, Substorm effects on spectral structures of Pc 1 waves at synchronous orbit, J. Geophys. Res., 92, 143, 1987.", - "Kennel, C. F., H. E. Petschek, Limit on stably trapped particle fluxes, J. Geophys. Res., 71, 1, 1966.", - "Kintner, P. M., D. A. Gurnett, Observations of ion cyclotron waves within the plasmaphere, J. Geophys. Res., 82, 2314, 1977.", - "Kozyra, J. U., T. E. Cravens, A. F. Nagy, E. G. Fontheim, Effects of energetic heavy ions on electromagnetic ion cyclotron wave generation in the plasmapause region, J. Geophys. Res, 89, 2217, 1984.", - "Krimigis, S. M., G. Gloeckler, R. W. McEntire, T. A. Potemera, F. L. Scarf, E. G. Shelley, Magnetic storm of September 4, 1984: A synthesis of ring current spectra and energy densities measured with AMPTE/CCE, Geophys. Res. Lett., 12, 329, 1985.", - "Ludlow, G. R., Growth of obliquely propagating ion cyclotron waves in the magnetosphere, J. Geophys. Res., 9415, 385, 1989.", - "Mauk, B. H., Helium resonance and dispersion effects on geostationary Alfven/ion cyclotron waves, J. Geophys. Res., 87, 9107, 1982a.", - "Mauk, B. H., Electromagnetic wave energization of heavy ions by the electric “phase bunching” process, Geophys. Res. Lett., 9, 1163, 1982b.", - "Mauk, B. H., Frequency gap formation in electromagnetic cyclotron wave distributions, Geophys. Res. Lett., 10, 635, 1983.", - "Mauk, B. H., C. E. McIlwain, R. L. McPherron, Helium cyclotron resonance within the Earth's magnetosphere, Geophys. Res. Lett., 8, 103, 1981.", - "Olsen, R. C., S. D. Shawhan, D. L. Gallagher, J. L. Green, C. R. Chappell, R. R. Anderson, Plasma observations at the Earth's magnetic equator, J. Geophys. Res., 92, 2385, 1987.", - "Perraut, S., R. Gendrin, A. Roux, Amplification of ion cyclotron waves for various typical radial profiles of magnetospheric parameters, J. Atmos. Terr. Phys., 38, 1191, 1976.", - "Perraut, S., R. Gendrin, A. Roux, C. deVilledary, Ion cyclotron waves: Direct comparison between ground‐based measurements and observations in the source region, J. Geophys. Res., 89, 195, 1984.", - "Rauch, J. L., A. Roux, Ray tracing of ULF waves in a multicomponent magnetospheric plasma: Consequences for the generation mechanism of ion cyclotron waves, J. Geophys. Res., 87, 8191, 1982.", - "Rönnmark, K., M. André, Convection of ion cyclotron waves to ion‐heating regions, J. Geophys. Res., 9617, 573, 1991.", - "Roux, A., S. Perraut, J. L. Rauch, C. deVilledary, Wave particle interactions near ΩHe observed on board GEOS 1 and 2, 2, generation of ion cyclotron waves and heating of He+ ions, J. Geophys. Res., 87, 8174, 1982.", - "Swanson, D. G., Plasma Waves, Academic, San Diego, Calif., 1989.", - "Sawada, A., Y. Kasahara, M. Yamamoto, I. Kimura, ELF emissions observed by the EXOS‐D satellite around the geomagnetic equatorial region, Geophys. Res. Lett., 18, 317, 1991.", - "Taylor, W. W. L., B. K. Paradt, L. J. Cahill Jr., Explorer 45 observations of 1‐ to 30‐Hz magnetic fields near the plasmapause during magnetic storms, J. Geophys. Res., 80, 1271, 1975.", - "Taylor, W. W. L., L. R. Lyons, Simultaneous equatorial observations of 1‐ to 30‐Hz waves and pitch‐angle distributions of ring current ions, J. Geophys. Res., 81, 6177, 1976.", - "Thorne, R. M., R. B. Horne, The contribution of ion‐cyclotron waves to electron heating and SAR‐arc excitation near the storm‐time plasmapause, Geophys. Res. Lett., 19, 417, 1992.", - "Thorne, R. M., R. B. Horne, Cyclotron absorption of ion‐ cyclotron waves at the bi‐ion frequency, Geophys. Res. Lett., 20, 317, 1993.", - "Wandzura, S., F. V. Coroniti, Nonconvective ion cyclotron instability, Planet Space Sci., 23, 123, 1975.", - "Williams, D. J., Ring current and radiation belts, Rev. of Geophys., 25, 570, 1987.", - "Young, D. T., S. Perraut, A. Roux, C. deVilledary, R. Gendrin, A. Korth, G. Kremser, D. Jones, Wave‐particle interactions near ΩHe+ observed on GEOS 1 and 2, 1, Propagation of ion cyclotron waves in a He+ rich plasma, J. Geophys. Res., 86, 6755, 1981."], - "title": {"textEnglish": "Convective instabilities of electromagnetic ion cyclotron waves in the outer magnetosphere"}} +{ + "abstract": { + "textEnglish": "The path\u2010integrated linear growth of electromagnetic ion cyclotron waves in the outer (L \u2265 7) magnetosphere is investigated using a realistic thermal plasma distribution with an additional anisotropic energetic ring current H+ to provide free energy for instability. The results provide a realistic simulation of the recent AMPTE observations. For conditions typical of the dayside magnetosphere, high plasma beta effects reduce the group velocity and significantly increase the spatial growth rates for left\u2010hand polarized instabilities just below the helium gyrofrequency \u03a9He+, and on the unguided mode above \u03a9>He+ but below the cross over frequency \u03c9cr. Relatively high densities, typical of the afternoon local time sector, favor these low group velocity effects for predominantly field\u2010aligned waves. Lower densities, typical of those found in the early morning local time sector, increase the group velocity but allow strong convective instabilities at high normalized frequencies well above \u03a9He+. These waves are reflected in the magnetosphere and can exist for several equatorial transits without significant damping. They are left\u2010hand polarized only on the first equatorial crossing and become linearly polarized for the remainder of the ray path. Consequently, these waves should be observed with basically linear polarization at all frequencies and all latitudes in the early morning local time sector. Wave growth below \u03a9He+ is severely limited owing to the narrow bandwidth for instability and the small resonant path lengths. In the afternoon sector, where plasma densities can exceed 107 m\u22123, intense convective amplification is possible both above and below \u03a9He+. Waves below \u03a9He+ are not subject to reflection when the O+ concentration is small and therefore should be observed with left\u2010hand polarization near the equator and essentially linear polarization at higher latitudes. Since the He+ concentration is usually large in the afternoon sector, guided mode waves above \u03a9He+ reflect to form a background distribution with basically linear polarization. We suggest that the strong left\u2010hand polarized emissions observed by AMPTE in the afternoon sector near the equator are probably due to strongly growing low group velocity waves at frequencies just below \u03a9He+, and on the unguided mode above \u03a9He+." + }, + "authors": [ + { + "name": { + "given_name": "Richard B.", + "surname": "Horne" + } + }, + { + "name": { + "given_name": "Richard M.", + "surname": "Thorne" + } + } + ], + "copyright": { + "statement": "Copyright 1994 by the American Geophysical Union.", + "status": true + }, + "editorialHistory": { + "acceptedDate": "1994-05-12", + "receivedDates": [ + "1993-05-24" + ] + }, + "pagination": { + "firstPage": "17259", + "lastPage": "17273", + "pageCount": "15" + }, + "persistentIDs": [ + { + "DOI": "10.1029/94JA01259" + } + ], + "pubDate": { + "electrDate": "2012-09-20", + "printDate": "1994-09-01" + }, + "publication": { + "ISSN": [ + { + "issnString": "0148-0227", + "pubtype": "print" + }, + { + "issnString": "2156-2202", + "pubtype": "electronic" + } + ], + "issueNum": "A9", + "pubName": "Journal of Geophysical Research: Space Physics", + "pubYear": "1994", + "volumeNum": "99" + }, + "publisherIDs": [ + { + "Identifier": "94JA01259", + "attribute": "editorialOffice" + }, + { + "Identifier": "JGRA12057", + "attribute": "unit" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + "Anderson, B. J., D. C. Hamilton, Electromagnetic ion cyclotron waves stimulated by modest magnetospheric compressions, J. Geophys. Res., 9811, 369, 1993.", + "Anderson, B. J., K. Takahashi, R. E. Erlandson, L. J. Zanetti, Pc1 pulsations observed by AMPTE/CCE in the Earth's outer magnetosphere, Geophys. Res. Lett., 17, 1853, 1990.", + "Anderson, B. J., R. E. Erlandson, L. J. Zanetti, A statistical study of Pc 1\u20132 magnetic pulsations in the equatorial magnetosphere, 1, Equatorial occurrence distributions, J. Geophys. Res., 97, 3075, 1992a.", + "Anderson, B. J., R. E. Erlandson, L. J. Zanetti, A statistical study of Pc 1\u20132 magnetic pulsations in the equatorial magnetosphere, 2, Wave properties, J. Geophys. Res., 97, 3089, 1992b.", + "Andr\u00e9, M., Dispersion surfaces, J. Plasma Phys., 33, 1, 1985.", + "Ashour\u2010 Abdalla, M., C. F. Kennel, Nonconvective and convective electron cyclotron harmonic instabilities, J. Geophys. Res., 83, 1531, 1978.", + "Bossen, M., R. L. McPherron, C. T. Russel, A statistical study of pc 1 magnetic pulsations at synchronous Orbit, J. Geophys. Res., 81, 6083, 1976.", + "Budden, K. G., The Propagation of Radio Waves, Cambridge University Press, New York, 1985.", + "Cornwall, J. M., F. V. Coroniti, R. M. Thorne, Turbulent loss of ring current protons, J. Geophys. Res., 75, 4699, 1970.", + "Cornwall, J. M., F. V. Coroniti, R. M. Thorne, Unified theory of SAR arc formation at the plasmapause, J. Geophys. Res., 76, 4428, 1971.", + "Denton, R. E., M. K. Hudson, I. Roth, Loss\u2010cone\u2010driven ion cyclotron waves in the magnetosphere, J. Geophys. Res., 9712, 093, 1992.", + "Fried, B. D., S. D. Conte, The Plasma Dispersion Function, Academic, San Diego, Calif., 1961.", + "Fraser, B. J., W. J. Kemp, D. J. Webster, Ground\u2010satellite study of a Pc 1 ion cyclotron wave event, J. Geophys. Res., 9411, 855, 1989.", + "Fraser, B. J., R. L. McPherron, Pc 1\u20132 magnetic pulsation spectra and heavy ion effects at synchronous orbit: ATS 6 results, J. Geophys. Res., 87, 4560, 1982.", + "Gendrin, R., A. Roux, Energization of helium ions by proton induced hydromagnetic waves, J. Geophys. Res., 85, 4577, 1980.", + "Gendrin, R., M. Ashour\u2010Abdalla, Y. Omura, K. Quest, Linear analysis of ion cyclotron interaction in a multicomponent plasma, J. Geophys. Res., 89, 9119, 1984.", + "Gloeckler, G., B. Wilken, W. Studemann, F. M. Ipavich, D. Hovestadt, D. C. Hamilton, G. Kremser, First composition measurement of the bulk of the storm time ring\u2010current (1 to 300 keV/e) with AMPTE\u2010CCE, Geophys. Res. Lett., 12, 325, 1985.", + "Gomberoff, L., R. Neira, Convective growth rate of ion cyclotron waves in a H+\u2010He+ and H+\u2010He+\u2010O+ plasma, J. Geophys. Res., 88, 2170, 1983.", + "Higel, B., L. Wu, Electron density and plasmapause characteristics at 6.6RE, A statistical study of the GEOS 2 relaxation sounder data, J. Geophys. Res., 89, 1583, 1984.", + "Horne, R. B., Path\u2010integrated growth of electrostatic waves: The generation of terrestrial myriametric radiation, J. Geophys. Res., 94, 8895, 1989.", + "Horne, R. B., R. M. Thorne, Ion cyclotron absorption at the second harmonic of the oxygen gyrofrequency, Geophys. Res. Lett., 17, 2225, 1990.", + "Horne, R. B., R. M. Thorne, On the preferred source location for the convective amplification of ion cyclotron waves, J. Geophys. Res., 98, 9233, 1993.", + "Hu, Y. D., B. J. Fraser, J. V. Olsen, Amplification of electromagnetic ion cyclotron waves along a wave path in the Earth's multi\u2010component magnetosphere, Geophys. Res., Lett., 17, 1053, 1990.", + "Hu, Y. D., B. J. Fraser, Electromagnetic ion cyclotron wave amplification and source regions in the magnetosphere, J. Geophys. Res., 99, 263, 1994.", + "Inan, U. S., T. F. Bell, The plasmapause as a VLF wave guide, J. Geophys. Res., 19, 2819, 1977.", + "Ishida, I., S. Kokubun, R. L. McPherron, Substorm effects on spectral structures of Pc 1 waves at synchronous orbit, J. Geophys. Res., 92, 143, 1987.", + "Kennel, C. F., H. E. Petschek, Limit on stably trapped particle fluxes, J. Geophys. Res., 71, 1, 1966.", + "Kintner, P. M., D. A. Gurnett, Observations of ion cyclotron waves within the plasmaphere, J. Geophys. Res., 82, 2314, 1977.", + "Kozyra, J. U., T. E. Cravens, A. F. Nagy, E. G. Fontheim, Effects of energetic heavy ions on electromagnetic ion cyclotron wave generation in the plasmapause region, J. Geophys. Res, 89, 2217, 1984.", + "Krimigis, S. M., G. Gloeckler, R. W. McEntire, T. A. Potemera, F. L. Scarf, E. G. Shelley, Magnetic storm of September 4, 1984: A synthesis of ring current spectra and energy densities measured with AMPTE/CCE, Geophys. Res. Lett., 12, 329, 1985.", + "Ludlow, G. R., Growth of obliquely propagating ion cyclotron waves in the magnetosphere, J. Geophys. Res., 9415, 385, 1989.", + "Mauk, B. H., Helium resonance and dispersion effects on geostationary Alfven/ion cyclotron waves, J. Geophys. Res., 87, 9107, 1982a.", + "Mauk, B. H., Electromagnetic wave energization of heavy ions by the electric \u201cphase bunching\u201d process, Geophys. Res. Lett., 9, 1163, 1982b.", + "Mauk, B. H., Frequency gap formation in electromagnetic cyclotron wave distributions, Geophys. Res. Lett., 10, 635, 1983.", + "Mauk, B. H., C. E. McIlwain, R. L. McPherron, Helium cyclotron resonance within the Earth's magnetosphere, Geophys. Res. Lett., 8, 103, 1981.", + "Olsen, R. C., S. D. Shawhan, D. L. Gallagher, J. L. Green, C. R. Chappell, R. R. Anderson, Plasma observations at the Earth's magnetic equator, J. Geophys. Res., 92, 2385, 1987.", + "Perraut, S., R. Gendrin, A. Roux, Amplification of ion cyclotron waves for various typical radial profiles of magnetospheric parameters, J. Atmos. Terr. Phys., 38, 1191, 1976.", + "Perraut, S., R. Gendrin, A. Roux, C. deVilledary, Ion cyclotron waves: Direct comparison between ground\u2010based measurements and observations in the source region, J. Geophys. Res., 89, 195, 1984.", + "Rauch, J. L., A. Roux, Ray tracing of ULF waves in a multicomponent magnetospheric plasma: Consequences for the generation mechanism of ion cyclotron waves, J. Geophys. Res., 87, 8191, 1982.", + "R\u00f6nnmark, K., M. Andr\u00e9, Convection of ion cyclotron waves to ion\u2010heating regions, J. Geophys. Res., 9617, 573, 1991.", + "Roux, A., S. Perraut, J. L. Rauch, C. deVilledary, Wave particle interactions near \u03a9He observed on board GEOS 1 and 2, 2, generation of ion cyclotron waves and heating of He+ ions, J. Geophys. Res., 87, 8174, 1982.", + "Swanson, D. G., Plasma Waves, Academic, San Diego, Calif., 1989.", + "Sawada, A., Y. Kasahara, M. Yamamoto, I. Kimura, ELF emissions observed by the EXOS\u2010D satellite around the geomagnetic equatorial region, Geophys. Res. Lett., 18, 317, 1991.", + "Taylor, W. W. L., B. K. Paradt, L. J. Cahill Jr., Explorer 45 observations of 1\u2010 to 30\u2010Hz magnetic fields near the plasmapause during magnetic storms, J. Geophys. Res., 80, 1271, 1975.", + "Taylor, W. W. L., L. R. Lyons, Simultaneous equatorial observations of 1\u2010 to 30\u2010Hz waves and pitch\u2010angle distributions of ring current ions, J. Geophys. Res., 81, 6177, 1976.", + "Thorne, R. M., R. B. Horne, The contribution of ion\u2010cyclotron waves to electron heating and SAR\u2010arc excitation near the storm\u2010time plasmapause, Geophys. Res. Lett., 19, 417, 1992.", + "Thorne, R. M., R. B. Horne, Cyclotron absorption of ion\u2010 cyclotron waves at the bi\u2010ion frequency, Geophys. Res. Lett., 20, 317, 1993.", + "Wandzura, S., F. V. Coroniti, Nonconvective ion cyclotron instability, Planet Space Sci., 23, 123, 1975.", + "Williams, D. J., Ring current and radiation belts, Rev. of Geophys., 25, 570, 1987.", + "Young, D. T., S. Perraut, A. Roux, C. deVilledary, R. Gendrin, A. Korth, G. Kremser, D. Jones, Wave\u2010particle interactions near \u03a9He+ observed on GEOS 1 and 2, 1, Propagation of ion cyclotron waves in a He+ rich plasma, J. Geophys. Res., 86, 6755, 1981." + ], + "title": { + "textEnglish": "Convective instabilities of electromagnetic ion cyclotron waves in the outer magnetosphere" + } +} diff --git a/tests/stubdata/output/wiley_jgra_57392.json b/tests/stubdata/output/wiley_jgra_57392.json index fb3c347..85d92a6 100644 --- a/tests/stubdata/output/wiley_jgra_57392.json +++ b/tests/stubdata/output/wiley_jgra_57392.json @@ -1,55 +1,274 @@ -{"abstract": {"textEnglish": "Abstract Whistler waves are often observed in magnetopause reconnection associated with electron beams. We analyze seven MMS crossings surrounding the electron diffusion region (EDR) to study the role of electron beams in whistler excitation. Waves have two major types: (a) Narrow‐band waves with high ellipticities and (b) broad‐band waves that are more electrostatic with significant variations in ellipticities and wave normal angles. While both types of waves are associated with electron beams, the key difference is the anisotropy of the background population, with perpendicular and parallel anisotropies, respectively. The linear instability analysis suggests that the first type of wave is mainly due to the background anisotropy, with the beam contributing additional cyclotron resonance to enhance the wave growth. The second type of broadband waves are excited via Landau resonance, and as seen in one event, the beam anisotropy induces an additional cyclotron mode. The results are supported by particle‐in‐cell simulations. We infer that the first type occurs downstream of the central EDR, where background electrons experience Betatron acceleration to form the perpendicular anisotropy; the second type occurs in the central EDR of guide field reconnection. A parametric study is conducted with linear instability analysis. A beam anisotropy alone of above ∼3 likely excites the cyclotron mode waves. Large beam drifts cause Doppler shifts and may lead to left‐hand polarizations in the ion frame. Future studies are needed to determine whether the observation covers a broader parameter regime and to understand the competition between whistler and other instabilities."}, - "authors": [{"affiliation": [{"affPubID": "jgra57392-aff-0001", "affPubRaw": "Astronomy Department, University of Maryland, College Park, MD, USA"}, {"affPubID": "jgra57392-aff-0002", "affPubRaw": "NASA Goddard Space Flight Center, Greenbelt, MD, USA"}], "attrib": {"email": "swang90@umd.edu", "orcid": "0000-0002-6783-7759"}, "name": {"given_name": "Shan", "surname": "Wang"}}, {"affiliation": [{"affPubID": "jgra57392-aff-0001", "affPubRaw": "Astronomy Department, University of Maryland, College Park, MD, USA"}, {"affPubID": "jgra57392-aff-0002", "affPubRaw": "NASA Goddard Space Flight Center, Greenbelt, MD, USA"}], "attrib": {"orcid": "0000-0002-5431-174X"}, "name": {"given_name": "Naoki", "surname": "Bessho"}}, {"affiliation": [{"affPubID": "jgra57392-aff-0003", "affPubRaw": "Swedish Institute of Space Physics, Uppsala, Sweden"}], "attrib": {"orcid": "0000-0002-1046-746X"}, "name": {"given_name": "Daniel B.", "surname": "Graham"}}, {"affiliation": [{"affPubID": "jgra57392-aff-0004", "affPubRaw": "Laboratoire de Physique des Plasmas, CNRS/Sorbonne Université/Université Paris‐Saclay/Observatoire de Paris/ Ecole Polytechnique Institut Polytechnique de Paris, Paris, France"}], "attrib": {"orcid": "0000-0003-2713-7966"}, "name": {"given_name": "Olivier", "surname": "Le Contel"}}, {"affiliation": [{"affPubID": "jgra57392-aff-0005", "affPubRaw": "Department of Physics, University of Texas at Arlington, Arlington, TX, USA"}], "name": {"given_name": "Frederick D.", "surname": "Wilder"}}, {"affiliation": [{"affPubID": "jgra57392-aff-0003", "affPubRaw": "Swedish Institute of Space Physics, Uppsala, Sweden"}], "attrib": {"orcid": "0000-0001-5550-3113"}, "name": {"given_name": "Yuri V.", "surname": "Khotyaintsev"}}, {"affiliation": [{"affPubID": "jgra57392-aff-0006", "affPubRaw": "Earth, Oceans, and Space Science, Southwest Research Institute, Durham, NH, USA"}], "attrib": {"orcid": "0000-0001-6890-2973"}, "name": {"given_name": "Kevin J.", "surname": "Genestreti"}}, {"affiliation": [{"affPubID": "jgra57392-aff-0007", "affPubRaw": "Institut de Recherche en Astrophysique et Planétologie, Université de Toulouse, Toulouse, France"}, {"affPubID": "jgra57392-aff-0008", "affPubRaw": "Centre National de la Recherche Scientifique, Toulouse, France"}], "attrib": {"orcid": "0000-0001-6807-8494"}, "name": {"given_name": "Benoit", "surname": "Lavraud"}}, {"affiliation": [{"affPubID": "jgra57392-aff-0001", "affPubRaw": "Astronomy Department, University of Maryland, College Park, MD, USA"}, {"affPubID": "jgra57392-aff-0002", "affPubRaw": "NASA Goddard Space Flight Center, Greenbelt, MD, USA"}], "name": {"given_name": "Seung", "surname": "Choi"}}, {"affiliation": [{"affPubID": "jgra57392-aff-0009", "affPubRaw": "Southwest Research Institute San Antonio, San Antonio, TX, USA"}], "attrib": {"orcid": "0000-0003-0452-8403"}, "name": {"given_name": "James L.", "surname": "Burch"}}], - "copyright": {"statement": "©2022. The Authors.", "status": true}, - "editorialHistory": {"acceptedDate": "2022-09-01", "receivedDates": ["2022-07-28"], "revisedDates": ["2022-08-26"]}, - "pagination": {"electronicID": "e2022JA030882", "firstPage": "2022JA030882", "pageCount": "21"}, - "persistentIDs": [{"DOI": "10.1029/2022JA030882"}], - "pubDate": {"electrDate": "2022-09-21", "printDate": "2022-09-00"}, - "publication": {"ISSN": [{"issnString": "2169-9380", "pubtype": "print"}, {"issnString": "2169-9402", "pubtype": "electronic"}], "issueNum": "9", "pubName": "Journal of Geophysical Research: Space Physics", "pubYear": "2022", "volumeNum": "127"}, - "publisherIDs": [{"Identifier": "JGRA57392", "attribute": "unit"}], - "recordData": {"createdTime": "", "loadFormat": "OtherXML", "loadLocation": "", "loadType": "fromFile", "parsedTime": "", "recordOrigin": ""}, - "references": ["Akimoto, K., Winske, D., Gary, S. P., & Thomsen, M. F. (1993). Nonlinear evolution of electromagnetic ion beam instabilities. Journal of Geophysical Research, 98(A2), 1419–1433. https://doi.org/10.1029/92JA02345", - "An, X., Van Compernolle, B., Bortnik, J., Thorne, R. M., Chen, L., & Li, W. (2016). Resonant excitation of whistler waves by a helical electron beam. Geophysical Research Letters, 43, 2413–2421. https://doi.org/10.1002/2015GL067126", - "Bessho, N., Chen, L.‐J., Wang, S., & Hesse, M. (2019). Effects of the guide field on electron distribution functions in the diffusion region of asymmetric reconnection. Physics of Plasmas, 26, 082310. https://doi.org/10.1063/1.5092809", - "Bowers, K. J., Albright, B. J., Bergen, B., Yin, L., Barker, K. J., & Kerbyson, D. J. (2008). 0.374 pflop/s trillion‐particle kinetic modeling of laser plasma interaction on roadrunner. In Proceedings of the 2008 ACM/IEEE Conference on Supercomputing SC '08 (pp. 63:1–63:11). IEEE Press. https://doi.org/10.1109/sc.2008.5222734", - "Burch, J. L., Ergun, R. E., Cassak, P. A., Webster, J. M., Torbert, R. B., Giles, B. L., et al. (2018). Localized oscillatory energy conversion in magnetopause reconnection. Geophysical Research Letters, 45, 1237–1245. https://doi.org/10.1002/2017GL076809", - "Burch, J. L., & Phan, T. D. (2016). Magnetic reconnection at the dayside magnetopause: Advances with MMS. Geophysical Research Letters, 43, 8327–8338. https://doi.org/10.1002/2016GL069787", - "Burch, J. L., Webster, J. M., Genestreti, K. J., Torbert, R. B., Giles, B. L., Fuselier, S. A., et al. (2018). Wave phenomena and beam‐plasma interactions at the magnetopause reconnection region. Journal of Geophysical Research: Space Physics, 123, 1118–1133. https://doi.org/10.1002/2017JA024789", - "Cao, D., Fu, H. S., Cao, J. B., Wang, T. Y., Graham, D. B., Chen, Z. Z., et al. (2017). MMS observations of whistler waves in electron diffusion region. Geophysical Research Letters, 44, 3954–3962. https://doi.org/10.1002/2017GL072703", - "Chen, H., Gao, X., Lu, Q., Fan, K., Ke, Y., Wang, X., & Wang, S. (2022). 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The nonlinear behavior of whistler waves at the reconnecting dayside magnetopause as observed by the magnetospheric multiscale mission: A case study. Journal of Geophysical Research: Space Physics, 122(5), 5487–5501. https://doi.org/10.1002/2017JA024062", - "Wong, H. K., & Smith, C. W. (1994). Electron beam excitation of upstream waves in the whistler mode frequency range. Journal of Geophysical Research, 99(A7), 13373–13387. https://doi.org/10.1029/94JA00821", - "Xie, H. (2019). BO: A unified tool for plasma waves and instabilities analysis. Computer Physics Communications, 244, 343–371. https://doi.org/10.1016/j.cpc.2019.06.014", - "Yoo, J., Jara‐Almonte, J., Yerger, E., Wang, S., Qian, T., Le, A., et al. (2018). Whistler wave generation by anisotropic tail electrons during asymmetric magnetic reconnection in space and laboratory. Geophysical Research Letters, 45, 8054–8061. https://doi.org/10.1029/2018GL079278", - "Zhao, S. Q., Xiao, C. J., Liu, T. Z., Chen, H., Zhang, H., Shi, M. J., et al. (2021). Observations of the beam‐driven whistler mode waves in the magnetic reconnection region at the dayside magnetopause. Journal of Geophysical Research: Space Physics, 126. https://doi.org/10.1029/2020JA028525", - "Zhong, Z. H., Graham, D. B., Khotyaintsev, Y. V., Zhou, M., Le Contel, O., Tang, R. X., & Deng, X. H. (2021). Whistler and broadband electrostatic waves in the multiple X‐line reconnection at the magnetopause. Geophysical Research Letters, 48, e2020GL091320. https://doi.org/10.1029/2020GL091320", - "Zhong, Z. H., Zhou, M., Graham, D. B., Khotyaintsev, Y. V., Wu, Y. F., Le Contel, O., et al. (2022). Evidence for whistler waves propagating into the electron diffusion region of collisionless magnetic reconnection. Geophysical Research Letters, 49, e2021GL097387. https://doi.org/10.1029/2021GL097387"], - "title": {"textEnglish": "Whistler Waves Associated With Electron Beams in Magnetopause Reconnection Diffusion Regions"}} +{ + "abstract": { + "textEnglish": "Abstract Whistler waves are often observed in magnetopause reconnection associated with electron beams. We analyze seven MMS crossings surrounding the electron diffusion region (EDR) to study the role of electron beams in whistler excitation. Waves have two major types: (a) Narrow\u2010band waves with high ellipticities and (b) broad\u2010band waves that are more electrostatic with significant variations in ellipticities and wave normal angles. While both types of waves are associated with electron beams, the key difference is the anisotropy of the background population, with perpendicular and parallel anisotropies, respectively. The linear instability analysis suggests that the first type of wave is mainly due to the background anisotropy, with the beam contributing additional cyclotron resonance to enhance the wave growth. The second type of broadband waves are excited via Landau resonance, and as seen in one event, the beam anisotropy induces an additional cyclotron mode. The results are supported by particle\u2010in\u2010cell simulations. We infer that the first type occurs downstream of the central EDR, where background electrons experience Betatron acceleration to form the perpendicular anisotropy; the second type occurs in the central EDR of guide field reconnection. A parametric study is conducted with linear instability analysis. A beam anisotropy alone of above \u223c3 likely excites the cyclotron mode waves. Large beam drifts cause Doppler shifts and may lead to left\u2010hand polarizations in the ion frame. Future studies are needed to determine whether the observation covers a broader parameter regime and to understand the competition between whistler and other instabilities." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "jgra57392-aff-0001", + "affPubRaw": "Astronomy Department, University of Maryland, College Park, MD, USA" + }, + { + "affPubID": "jgra57392-aff-0002", + "affPubRaw": "NASA Goddard Space Flight Center, Greenbelt, MD, USA" + } + ], + "attrib": { + "email": "swang90@umd.edu", + "orcid": "0000-0002-6783-7759" + }, + "name": { + "given_name": "Shan", + "surname": "Wang" + } + }, + { + "affiliation": [ + { + "affPubID": "jgra57392-aff-0001", + "affPubRaw": "Astronomy Department, University of Maryland, College Park, MD, USA" + }, + { + "affPubID": "jgra57392-aff-0002", + "affPubRaw": "NASA Goddard Space Flight Center, Greenbelt, MD, USA" + } + ], + "attrib": { + "orcid": "0000-0002-5431-174X" + }, + "name": { + "given_name": "Naoki", + "surname": "Bessho" + } + }, + { + "affiliation": [ + { + "affPubID": "jgra57392-aff-0003", + "affPubRaw": "Swedish Institute of Space Physics, Uppsala, Sweden" + } + ], + "attrib": { + "orcid": "0000-0002-1046-746X" + }, + "name": { + "given_name": "Daniel B.", + "surname": "Graham" + } + }, + { + "affiliation": [ + { + "affPubID": "jgra57392-aff-0004", + "affPubRaw": "Laboratoire de Physique des Plasmas, CNRS/Sorbonne Universit\u00e9/Universit\u00e9 Paris\u2010Saclay/Observatoire de Paris/ Ecole Polytechnique Institut Polytechnique de Paris, Paris, France" + } + ], + "attrib": { + "orcid": "0000-0003-2713-7966" + }, + "name": { + "given_name": "Olivier", + "surname": "Le Contel" + } + }, + { + "affiliation": [ + { + "affPubID": "jgra57392-aff-0005", + "affPubRaw": "Department of Physics, University of Texas at Arlington, Arlington, TX, USA" + } + ], + "name": { + "given_name": "Frederick D.", + "surname": "Wilder" + } + }, + { + "affiliation": [ + { + "affPubID": "jgra57392-aff-0003", + "affPubRaw": "Swedish Institute of Space Physics, Uppsala, Sweden" + } + ], + "attrib": { + "orcid": "0000-0001-5550-3113" + }, + "name": { + "given_name": "Yuri V.", + "surname": "Khotyaintsev" + } + }, + { + "affiliation": [ + { + "affPubID": "jgra57392-aff-0006", + "affPubRaw": "Earth, Oceans, and Space Science, Southwest Research Institute, Durham, NH, USA" + } + ], + "attrib": { + "orcid": "0000-0001-6890-2973" + }, + "name": { + "given_name": "Kevin J.", + "surname": "Genestreti" + } + }, + { + "affiliation": [ + { + "affPubID": "jgra57392-aff-0007", + "affPubRaw": "Institut de Recherche en Astrophysique et Plan\u00e9tologie, Universit\u00e9 de Toulouse, Toulouse, France" + }, + { + "affPubID": "jgra57392-aff-0008", + "affPubRaw": "Centre National de la Recherche Scientifique, Toulouse, France" + } + ], + "attrib": { + "orcid": "0000-0001-6807-8494" + }, + "name": { + "given_name": "Benoit", + "surname": "Lavraud" + } + }, + { + "affiliation": [ + { + "affPubID": "jgra57392-aff-0001", + "affPubRaw": "Astronomy Department, University of Maryland, College Park, MD, USA" + }, + { + "affPubID": "jgra57392-aff-0002", + "affPubRaw": "NASA Goddard Space Flight Center, Greenbelt, MD, USA" + } + ], + "name": { + "given_name": "Seung", + "surname": "Choi" + } + }, + { + "affiliation": [ + { + "affPubID": "jgra57392-aff-0009", + "affPubRaw": "Southwest Research Institute San Antonio, San Antonio, TX, USA" + } + ], + "attrib": { + "orcid": "0000-0003-0452-8403" + }, + "name": { + "given_name": "James L.", + "surname": "Burch" + } + } + ], + "copyright": { + "statement": "\u00a92022. The Authors.", + "status": true + }, + "editorialHistory": { + "acceptedDate": "2022-09-01", + "receivedDates": [ + "2022-07-28" + ], + "revisedDates": [ + "2022-08-26" + ] + }, + "pagination": { + "electronicID": "e2022JA030882", + "firstPage": "2022JA030882", + "pageCount": "21" + }, + "persistentIDs": [ + { + "DOI": "10.1029/2022JA030882" + } + ], + "pubDate": { + "electrDate": "2022-09-21", + "printDate": "2022-09-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "2169-9380", + "pubtype": "print" + }, + { + "issnString": "2169-9402", + "pubtype": "electronic" + } + ], + "issueNum": "9", + "pubName": "Journal of Geophysical Research: Space Physics", + "pubYear": "2022", + "volumeNum": "127" + }, + "publisherIDs": [ + { + "Identifier": "JGRA57392", + "attribute": "unit" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + "Akimoto, K., Winske, D., Gary, S. 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In this study, a comparison of the predicted arrival times and speeds for each CME based, independently, on the inputs from the two STEREO vantage points is carried out. We perform hindcasts using ELlipse Evolution model based on Heliospheric Imager observations (ELEvoHI) ensemble modeling. An estimate of the ambient solar wind conditions is obtained by the Wang‐Sheeley‐Arge/Heliospheric Upwind eXtrapolation (WSA/HUX) model combination that serves as input to ELEvoHI. We carefully select 12 CMEs between February 2010 and July 2012 that show clear signatures in both STEREO‐A and STEREO‐B HI time‐elongation maps, that propagate close to the ecliptic plane, and that have corresponding in situ signatures at Earth. We find a mean arrival time difference of 6.5 h between predictions from the two different viewpoints, which can reach up to 9.5 h for individual CMEs, while the mean arrival speed difference is 63 km s−1. An ambient solar wind with a large speed variance leads to larger differences in the STEREO‐A and STEREO‐B CME arrival time predictions (cc = 0.92). Additionally, we compare the predicted arrivals, from both spacecraft, to the actual in situ arrivals at Earth and find a mean absolute error of 7.5 ± 9.5 h for the arrival time and 87 ± 111 km s−1 for the arrival speed. There is no tendency for one spacecraft to provide more accurate arrival predictions than the other."}, - "authors": [{"affiliation": [{"affPubID": "swe21103-aff-0001", "affPubRaw": "Space Research Institute, Austrian Academy of Sciences, Graz, Austria"}, {"affPubID": "swe21103-aff-0002", "affPubRaw": "Institute of Physics, University of Graz, Graz, Austria"}], "attrib": {"email": "juergen.hinterreiter@oeaw.ac.at", "orcid": "0000-0002-1222-8243"}, "name": {"given_name": "Jürgen", "surname": "Hinterreiter"}}, {"affiliation": [{"affPubID": "swe21103-aff-0001", "affPubRaw": "Space Research Institute, Austrian Academy of Sciences, Graz, Austria"}], "attrib": {"orcid": "0000-0001-9024-6706"}, "name": {"given_name": "Tanja", "surname": "Amerstorfer"}}, {"affiliation": [{"affPubID": "swe21103-aff-0001", "affPubRaw": "Space Research Institute, Austrian Academy of Sciences, Graz, Austria"}, {"affPubID": "swe21103-aff-0003", "affPubRaw": "Institute of Geodesy, Graz University of Technology, Graz, Austria"}], "attrib": {"orcid": "0000-0002-6362-5054"}, "name": {"given_name": "Martin A.", "surname": "Reiss"}}, {"affiliation": [{"affPubID": "swe21103-aff-0001", "affPubRaw": "Space Research Institute, Austrian Academy of Sciences, Graz, Austria"}, {"affPubID": "swe21103-aff-0003", "affPubRaw": "Institute of Geodesy, Graz University of Technology, Graz, Austria"}], "attrib": {"orcid": "0000-0001-6868-4152"}, "name": {"given_name": "Christian", "surname": "Möstl"}}, {"affiliation": [{"affPubID": "swe21103-aff-0002", "affPubRaw": "Institute of Physics, University of Graz, Graz, Austria"}], "attrib": {"orcid": "0000-0003-4867-7558"}, "name": {"given_name": "Manuela", "surname": "Temmer"}}, {"affiliation": [{"affPubID": "swe21103-aff-0001", "affPubRaw": "Space Research Institute, Austrian Academy of Sciences, Graz, Austria"}, {"affPubID": "swe21103-aff-0002", "affPubRaw": "Institute of Physics, University of Graz, Graz, Austria"}], "attrib": {"orcid": "0000-0002-2507-7616"}, "name": {"given_name": "Maike", "surname": "Bauer"}}, {"affiliation": [{"affPubID": "swe21103-aff-0001", "affPubRaw": "Space Research Institute, Austrian Academy of Sciences, Graz, Austria"}], "attrib": {"orcid": "0000-0003-1516-5441"}, "name": {"given_name": "Ute V.", "surname": "Amerstorfer"}}, {"affiliation": [{"affPubID": "swe21103-aff-0004", "affPubRaw": "Conrad Observatory, Zentralanstalt für Meteorologie und Geodynamik, Vienna, Austria"}], "attrib": {"orcid": "0000-0003-2021-6557"}, "name": {"given_name": "Rachel L.", "surname": "Bailey"}}, {"affiliation": [{"affPubID": "swe21103-aff-0001", "affPubRaw": "Space Research Institute, Austrian Academy of Sciences, Graz, Austria"}, {"affPubID": "swe21103-aff-0002", "affPubRaw": "Institute of Physics, University of Graz, Graz, Austria"}, {"affPubID": "swe21103-aff-0003", "affPubRaw": "Institute of Geodesy, Graz University of Technology, Graz, Austria"}], "attrib": {"orcid": "0000-0002-6273-4320"}, "name": {"given_name": "Andreas J.", "surname": "Weiss"}}, {"affiliation": [{"affPubID": "swe21103-aff-0005", "affPubRaw": "RAL Space, Rutherford Appleton Laboratory, Didcot, UK"}], "attrib": {"orcid": "0000-0001-9865-9281"}, "name": {"given_name": "Jackie A.", "surname": "Davies"}}, {"affiliation": [{"affPubID": "swe21103-aff-0006", "affPubRaw": "Department of Meteorology, University of Reading, Reading, UK"}], "attrib": {"orcid": "0000-0001-9876-4612"}, "name": {"given_name": "Luke A.", "surname": "Barnard"}}, {"affiliation": [{"affPubID": "swe21103-aff-0006", "affPubRaw": "Department of Meteorology, University of Reading, Reading, UK"}], "attrib": {"orcid": "0000-0003-2061-2453"}, "name": {"given_name": "Mathew J.", "surname": "Owens"}}], - "copyright": {"statement": "© 2021. The Authors.", "status": true}, - "editorialHistory": {"acceptedDate": "2021-01-29", "receivedDates": ["2020-10-30"], "revisedDates": ["2020-12-23"]}, - "pagination": {"electronicID": "e2020SW002674", "firstPage": "2020SW002674", "pageCount": "18"}, - "persistentIDs": [{"DOI": "10.1029/2020SW002674"}], - "pubDate": {"electrDate": "2021-03-26", "printDate": "2021-03-00"}, - "publication": {"ISSN": [{"issnString": "1542-7390", "pubtype": "print"}, {"issnString": "1542-7390", "pubtype": "electronic"}], "issueNum": "3", "pubName": "Space Weather", "pubYear": "2021", "volumeNum": "19"}, - "publisherIDs": [{"Identifier": "SWE21103", "attribute": "unit"}], - "recordData": {"createdTime": "", "loadFormat": "OtherXML", "loadLocation": "", "loadType": "fromFile", "parsedTime": "", "recordOrigin": ""}, - "references": ["Altschuler, M. D., & Newkirk, G. (1969). Magnetic fields and the structure of the solar corona. I: Methods of calculating coronal fields. 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An estimate of the ambient solar wind conditions is obtained by the Wang\u2010Sheeley\u2010Arge/Heliospheric Upwind eXtrapolation (WSA/HUX) model combination that serves as input to ELEvoHI. We carefully select 12 CMEs between February 2010 and July 2012 that show clear signatures in both STEREO\u2010A and STEREO\u2010B HI time\u2010elongation maps, that propagate close to the ecliptic plane, and that have corresponding in situ signatures at Earth. We find a mean arrival time difference of 6.5 h between predictions from the two different viewpoints, which can reach up to 9.5 h for individual CMEs, while the mean arrival speed difference is 63 km s\u22121. An ambient solar wind with a large speed variance leads to larger differences in the STEREO\u2010A and STEREO\u2010B CME arrival time predictions (cc = 0.92). Additionally, we compare the predicted arrivals, from both spacecraft, to the actual in situ arrivals at Earth and find a mean absolute error of 7.5 \u00b1 9.5 h for the arrival time and 87 \u00b1 111 km s\u22121 for the arrival speed. There is no tendency for one spacecraft to provide more accurate arrival predictions than the other." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "swe21103-aff-0001", + "affPubRaw": "Space Research Institute, Austrian Academy of Sciences, Graz, Austria" + }, + { + "affPubID": "swe21103-aff-0002", + "affPubRaw": "Institute of Physics, University of Graz, Graz, Austria" + } + ], + "attrib": { + "email": "juergen.hinterreiter@oeaw.ac.at", + "orcid": "0000-0002-1222-8243" + }, + "name": { + "given_name": "J\u00fcrgen", + "surname": "Hinterreiter" + } + }, + { + "affiliation": [ + { + "affPubID": "swe21103-aff-0001", + "affPubRaw": "Space Research Institute, Austrian Academy of Sciences, Graz, Austria" + } + ], + "attrib": { + "orcid": "0000-0001-9024-6706" + }, + "name": { + "given_name": "Tanja", + "surname": "Amerstorfer" + } + }, + { + "affiliation": [ + { + "affPubID": "swe21103-aff-0001", + "affPubRaw": "Space Research Institute, Austrian Academy of Sciences, Graz, Austria" + }, + { + "affPubID": "swe21103-aff-0003", + "affPubRaw": "Institute of Geodesy, Graz University of Technology, Graz, Austria" + } + ], + "attrib": { + "orcid": "0000-0002-6362-5054" + }, + "name": { + "given_name": "Martin A.", + "surname": "Reiss" + } + }, + { + "affiliation": [ + { + "affPubID": "swe21103-aff-0001", + "affPubRaw": "Space Research Institute, Austrian Academy of Sciences, Graz, Austria" + }, + { + "affPubID": "swe21103-aff-0003", + "affPubRaw": "Institute of Geodesy, Graz University of Technology, Graz, Austria" + } + ], + "attrib": { + "orcid": "0000-0001-6868-4152" + }, + "name": { + "given_name": "Christian", + "surname": "M\u00f6stl" + } + }, + { + "affiliation": [ + { + "affPubID": "swe21103-aff-0002", + "affPubRaw": "Institute of Physics, University of Graz, Graz, Austria" + } + ], + "attrib": { + "orcid": "0000-0003-4867-7558" + }, + "name": { + "given_name": "Manuela", + "surname": "Temmer" + } + }, + { + "affiliation": [ + { + "affPubID": "swe21103-aff-0001", + "affPubRaw": "Space Research Institute, Austrian Academy of Sciences, Graz, Austria" + }, + { + "affPubID": "swe21103-aff-0002", + "affPubRaw": "Institute of Physics, University of Graz, Graz, Austria" + } + ], + "attrib": { + "orcid": "0000-0002-2507-7616" + }, + "name": { + "given_name": "Maike", + "surname": "Bauer" + } + }, + { + "affiliation": [ + { + "affPubID": "swe21103-aff-0001", + "affPubRaw": "Space Research Institute, Austrian Academy of Sciences, Graz, Austria" + } + ], + "attrib": { + "orcid": "0000-0003-1516-5441" + }, + "name": { + "given_name": "Ute V.", + "surname": "Amerstorfer" + } + }, + { + "affiliation": [ + { + "affPubID": "swe21103-aff-0004", + "affPubRaw": "Conrad Observatory, Zentralanstalt f\u00fcr Meteorologie und Geodynamik, Vienna, Austria" + } + ], + "attrib": { + "orcid": "0000-0003-2021-6557" + }, + "name": { + "given_name": "Rachel L.", + "surname": "Bailey" + } + }, + { + "affiliation": [ + { + "affPubID": "swe21103-aff-0001", + "affPubRaw": "Space Research Institute, Austrian Academy of Sciences, Graz, Austria" + }, + { + "affPubID": "swe21103-aff-0002", + "affPubRaw": "Institute of Physics, University of Graz, Graz, Austria" + }, + { + "affPubID": "swe21103-aff-0003", + "affPubRaw": "Institute of Geodesy, Graz University of Technology, Graz, Austria" + } + ], + "attrib": { + "orcid": "0000-0002-6273-4320" + }, + "name": { + "given_name": "Andreas J.", + "surname": "Weiss" + } + }, + { + "affiliation": [ + { + "affPubID": "swe21103-aff-0005", + "affPubRaw": "RAL Space, Rutherford Appleton Laboratory, Didcot, UK" + } + ], + "attrib": { + "orcid": "0000-0001-9865-9281" + }, + "name": { + "given_name": "Jackie A.", + "surname": "Davies" + } + }, + { + "affiliation": [ + { + "affPubID": "swe21103-aff-0006", + "affPubRaw": "Department of Meteorology, University of Reading, Reading, UK" + } + ], + "attrib": { + "orcid": "0000-0001-9876-4612" + }, + "name": { + "given_name": "Luke A.", + "surname": "Barnard" + } + }, + { + "affiliation": [ + { + "affPubID": "swe21103-aff-0006", + "affPubRaw": "Department of Meteorology, University of Reading, Reading, UK" + } + ], + "attrib": { + "orcid": "0000-0003-2061-2453" + }, + "name": { + "given_name": "Mathew J.", + "surname": "Owens" + } + } + ], + "copyright": { + "statement": "\u00a9 2021. The Authors.", + "status": true + }, + "editorialHistory": { + "acceptedDate": "2021-01-29", + "receivedDates": [ + "2020-10-30" + ], + "revisedDates": [ + "2020-12-23" + ] + }, + "pagination": { + "electronicID": "e2020SW002674", + "firstPage": "2020SW002674", + "pageCount": "18" + }, + "persistentIDs": [ + { + "DOI": "10.1029/2020SW002674" + } + ], + "pubDate": { + "electrDate": "2021-03-26", + "printDate": "2021-03-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "1542-7390", + "pubtype": "print" + }, + { + "issnString": "1542-7390", + "pubtype": "electronic" + } + ], + "issueNum": "3", + "pubName": "Space Weather", + "pubYear": "2021", + "volumeNum": "19" + }, + "publisherIDs": [ + { + "Identifier": "SWE21103", + "attribute": "unit" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + "Altschuler, M. D., & Newkirk, G. (1969). 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Solar Physics, 222(2), 329\u2013343. https://doi.org/10.1023/B:SOLA.0000043576.21942.aa", + "Wang, Y., Wang, B., Shen, C., Shen, F., & Lugaz, N. (2014). Deflected propagation of a coronal mass ejection from the corona to interplanetary space. Journal of Geophysical Research: Space Physics, 119, 5117\u20135132. https://doi.org/10.1002/2013JA019537", + "Wang, Y.\u2010M., & Sheeley, N. R. Jr. (1995). Solar implications of ULYSSES interplanetary field measurements. The Astrophysical Journal Letters, 447, L143. https://doi.org/10.1086/309578", + "\u017dic, T., Vr\u0161nak, B., & Temmer, M. (2015). Heliospheric propagation of coronal mass ejections: Drag\u2010based model fitting. The Astrophysical Journal Supplement Series, 218(2), 32. https://doi.org/10.1088/0067\u20100049/218/2/32", + "Zuccarello, F. P., Bemporad, A., Jacobs, C., Mierla, M., Poedts, S., & Zuccarello, F. (2012). The role of streamers in the deflection of coronal mass ejections: Comparison between STEREO three\u2010dimensional reconstructions and numerical simulations. The Astrophysical Journal, 744(1), 66. https://doi.org/10.1088/0004\u2010637X/744/1/66" + ], + "title": { + "textEnglish": "Why are ELEvoHI CME Arrival Predictions Different if Based on STEREO\u2010A or STEREO\u2010B Heliospheric Imager Observations?" + } +} diff --git a/tests/stubdata/output/wiley_swe_461.json b/tests/stubdata/output/wiley_swe_461.json index 218893f..ecae406 100644 --- a/tests/stubdata/output/wiley_swe_461.json +++ b/tests/stubdata/output/wiley_swe_461.json @@ -1 +1,73 @@ -{"abstract": {"textEnglish": "Geomagnetically induced currents (GICs) from solar storms pose a risk to the operation of power transmission grids in Europe and across the globe. The European Risk from Geomagnetically Induced Currents (EURISGIC) project, which began in March 2011 and is supported by the Seventh Framework Programme of the European Union, seeks to mitigate this natural hazard by developing European capabilities for GIC forecasting and warning. Recent well‐recognized GIC events were the province‐wide blackout in Quebec, Canada, in March 1989 and the blackout in the city of Malmö, in southern Sweden, during the Halloween storm of October 2003. The progressive integration of interconnected and geographically wide power transmission grids is obviously increasing the GIC risk. Hence, there is a need for greater scientific understanding of phenomena in the solar‐terrestrial environment that lead to GICs and for the development of systems that facilitate GIC modeling, forecasting, and mitigation."}, "authors": [{"affiliation": [{"affPubID": "swe461-aff-0001", "affPubRaw": "Senior scientist at the Finnish Meteorological Institute, in Helsinki, Finland. 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The European Risk from Geomagnetically Induced Currents (EURISGIC) project, which began in March 2011 and is supported by the Seventh Framework Programme of the European Union, seeks to mitigate this natural hazard by developing European capabilities for GIC forecasting and warning. Recent well\u2010recognized GIC events were the province\u2010wide blackout in Quebec, Canada, in March 1989 and the blackout in the city of Malm\u00f6, in southern Sweden, during the Halloween storm of October 2003. The progressive integration of interconnected and geographically wide power transmission grids is obviously increasing the GIC risk. Hence, there is a need for greater scientific understanding of phenomena in the solar\u2010terrestrial environment that lead to GICs and for the development of systems that facilitate GIC modeling, forecasting, and mitigation." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "swe461-aff-0001", + "affPubRaw": "Senior scientist at the Finnish Meteorological Institute, in Helsinki, Finland. E\u2010mail: ari.viljanen@fmi.fi" + } + ], + "name": { + "given_name": "Ari", + "surname": "Viljanen" + } + } + ], + "copyright": { + "statement": "Copyright 2011 by the American Geophysical Union.", + "status": true + }, + "pagination": { + "firstPage": "S07007", + "pageCount": "2" + }, + "persistentIDs": [ + { + "DOI": "10.1029/2011SW000680" + } + ], + "pubDate": { + "electrDate": "2011-07-28", + "printDate": "2011-07-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "1542-7390", + "pubtype": "print" + }, + { + "issnString": "1542-7390", + "pubtype": "electronic" + } + ], + "issueNum": "7", + "pubName": "Space Weather", + "pubYear": "2011", + "volumeNum": "9" + }, + "publisherIDs": [ + { + "Identifier": "2011SW000680", + "attribute": "editorialOffice" + }, + { + "Identifier": "SWE461", + "attribute": "unit" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "title": { + "textEnglish": "European Project to Improve Models of Geomagnetically Induced Currents" + } +} diff --git a/tests/stubdata/output/wiley_swe_539.json b/tests/stubdata/output/wiley_swe_539.json index c94fa90..1e95001 100644 --- a/tests/stubdata/output/wiley_swe_539.json +++ b/tests/stubdata/output/wiley_swe_539.json @@ -1 +1,73 @@ -{"abstract": {"textEnglish": "Delores Knipp's textbook Understanding Space Weather and the Physics Behind It provides a comprehensive resource for space physicists teaching in a variety of academic departments to introduce space weather to advanced undergraduates. The book benefits from Knipp's extensive experience teaching introductory and advanced undergraduate physics courses at the U.S. Air Force Academy. The fundamental physics concepts are clearly explained and are connected directly to the space physics concepts being discussed. To expand upon the relevant basic physics, current research areas and new observations are highlighted, with many of the chapters including contributions from a number of leading space physicists."}, "authors": [{"affiliation": [{"affPubID": "swe539-aff-0001", "affPubRaw": "University of Michigan USA"}], "name": {"given_name": "Mark", "surname": "Moldwin"}}], "copyright": {"statement": "©2012. American Geophysical Union. All Rights Reserved.", "status": true}, "pagination": {"firstPage": "S08004", "pageCount": "2"}, "persistentIDs": [{"DOI": "10.1029/2012SW000823"}], "pubDate": {"electrDate": "2012-08-03", "printDate": "2012-08-00"}, "publication": {"ISSN": [{"issnString": "1542-7390", "pubtype": "print"}, {"issnString": "1542-7390", "pubtype": "electronic"}], "issueNum": "8", "pubName": "Space Weather", "pubYear": "2012", "volumeNum": "10"}, "publisherIDs": [{"Identifier": "2012SW000823", "attribute": "editorialOffice"}, {"Identifier": "SWE539", "attribute": "unit"}], "recordData": {"createdTime": "", "loadFormat": "OtherXML", "loadLocation": "", "loadType": "fromFile", "parsedTime": "", "recordOrigin": ""}, "title": {"textEnglish": "Book Review: Dolores Knipp's Understanding Space Weather and the Physics Behind It"}} +{ + "abstract": { + "textEnglish": "Delores Knipp's textbook Understanding Space Weather and the Physics Behind It provides a comprehensive resource for space physicists teaching in a variety of academic departments to introduce space weather to advanced undergraduates. The book benefits from Knipp's extensive experience teaching introductory and advanced undergraduate physics courses at the U.S. Air Force Academy. The fundamental physics concepts are clearly explained and are connected directly to the space physics concepts being discussed. To expand upon the relevant basic physics, current research areas and new observations are highlighted, with many of the chapters including contributions from a number of leading space physicists." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "swe539-aff-0001", + "affPubRaw": "University of Michigan USA" + } + ], + "name": { + "given_name": "Mark", + "surname": "Moldwin" + } + } + ], + "copyright": { + "statement": "\u00a92012. American Geophysical Union. All Rights Reserved.", + "status": true + }, + "pagination": { + "firstPage": "S08004", + "pageCount": "2" + }, + "persistentIDs": [ + { + "DOI": "10.1029/2012SW000823" + } + ], + "pubDate": { + "electrDate": "2012-08-03", + "printDate": "2012-08-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "1542-7390", + "pubtype": "print" + }, + { + "issnString": "1542-7390", + "pubtype": "electronic" + } + ], + "issueNum": "8", + "pubName": "Space Weather", + "pubYear": "2012", + "volumeNum": "10" + }, + "publisherIDs": [ + { + "Identifier": "2012SW000823", + "attribute": "editorialOffice" + }, + { + "Identifier": "SWE539", + "attribute": "unit" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "title": { + "textEnglish": "Book Review: Dolores Knipp's Understanding Space Weather and the Physics Behind It" + } +} diff --git a/tests/stubdata/output/zenodo_test.json b/tests/stubdata/output/zenodo_test.json index 2d5cd52..291ccbd 100644 --- a/tests/stubdata/output/zenodo_test.json +++ b/tests/stubdata/output/zenodo_test.json @@ -1,19 +1,35 @@ { - 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Rodr\u00edguez", + "surname": "Rodr\u00edguez" + } }, { - "name": { - "surname": "de la Puente Gonz\u00e1lez", - "given_name": "Salvador", - "pubraw": "Salvador de la Puente Gonz\u00e1lez" - }, "affiliation": [ { "affPubRaw": "@IBMResearch" } - ] + ], + "name": { + "given_name": "Salvador", + "pubraw": "Salvador de la Puente Gonz\u00e1lez", + "surname": "de la Puente Gonz\u00e1lez" + } }, { - "name": { - "surname": "Nation", - "given_name": "Paul", - "pubraw": "Paul Nation" - }, "affiliation": [ { "affPubRaw": "IBM" } - ] + ], + "name": { + "given_name": "Paul", + "pubraw": "Paul Nation", + "surname": "Nation" + } }, { - "name": { - "surname": "Hu", - "given_name": "Shaohan", - "pubraw": "Shaohan Hu" - }, "affiliation": [ { "affPubRaw": "IBM Research" } - ] + ], + "name": { + "given_name": "Shaohan", + "pubraw": "Shaohan Hu", + "surname": "Hu" + } }, { - "name": { - "surname": "Zdanski", - "given_name": "Laura", - "pubraw": "Laura Zdanski" - }, "affiliation": [ { "affPubRaw": "@IBM @openliberty" } - ] + ], + "name": { + "given_name": "Laura", + "pubraw": "Laura Zdanski", + "surname": "Zdanski" + } }, { - "name": { - "surname": "Pistoia", - "given_name": "Marco", - "pubraw": "Marco Pistoia" - }, "affiliation": [ { "affPubRaw": "IBM" } - ] + ], + "name": { + "given_name": "Marco", + "pubraw": "Marco Pistoia", + "surname": "Pistoia" + } }, { "name": { - "surname": "Krsulich", "given_name": "Kevin", - "pubraw": "Kevin Krsulich" + "pubraw": "Kevin Krsulich", + "surname": "Krsulich" } }, { - "name": { - "given_name": "Travis-S-IBM", - "pubraw": "Travis-S-IBM" - }, "affiliation": [ { "affPubRaw": "IBM" } - ] + ], + "name": { + "given_name": "Travis-S-IBM", + "pubraw": "Travis-S-IBM" + } }, { "name": { - "surname": "Gomez", "given_name": "Juan", - "pubraw": "Juan Gomez" + "pubraw": "Juan Gomez", + "surname": "Gomez" } }, { - "name": { - "surname": "McKay", - "given_name": "David", - "pubraw": "David McKay" - }, "affiliation": [ { "affPubRaw": "@IBM, @Qiskit" } - ] + ], + "name": { + "given_name": "David", + "pubraw": "David McKay", + "surname": "McKay" + } }, { - "name": { - "surname": "Frisch", - "given_name": "Albert", - "pubraw": "Albert Frisch" - }, "affiliation": [ { "affPubRaw": "IBM @QISKit" } - ] + ], + "name": { + "given_name": "Albert", + "pubraw": "Albert Frisch", + "surname": "Frisch" + } }, { - "name": { - "surname": "Naveh", - "given_name": "Yehuda", - "pubraw": "Yehuda Naveh" - }, "affiliation": [ { "affPubRaw": "IBM Research" } - ] + ], + "name": { + "given_name": "Yehuda", + "pubraw": "Yehuda Naveh", + "surname": "Naveh" + } }, { - "name": { - "surname": "Wood", - "given_name": "Steve", - "pubraw": "Steve Wood" - }, "affiliation": [ { "affPubRaw": "IBM Research" } - ] + ], + "name": { + "given_name": "Steve", + "pubraw": "Steve Wood", + "surname": "Wood" + } }, { "name": { @@ -226,16 +193,16 @@ } }, { - "name": { - "surname": "Garion", - "given_name": "Shelly", - "pubraw": "Shelly Garion" - }, "affiliation": [ { "affPubRaw": "IBM" } - ] + ], + "name": { + "given_name": "Shelly", + "pubraw": "Shelly Garion", + "surname": "Garion" + } }, { "name": { @@ -250,16 +217,16 @@ } }, { - "name": { - "surname": "Cruz-Benito", - "given_name": "Juan", - "pubraw": "Juan Cruz-Benito" - }, "affiliation": [ { "affPubRaw": "@IBMResearch" } - ] + ], + "name": { + "given_name": "Juan", + "pubraw": "Juan Cruz-Benito", + "surname": "Cruz-Benito" + } }, { "name": { @@ -269,42 +236,42 @@ }, { "name": { - "surname": "Varchon", "given_name": "Francois", - "pubraw": "Francois Varchon" + "pubraw": "Francois Varchon", + "surname": "Varchon" } }, { - "name": { - "surname": "Wood", - "given_name": "Christopher", - "middle_name": "J.", - "pubraw": "Christopher J. Wood" - }, "affiliation": [ { "affPubRaw": "IBM Research @QISKit" } - ] + ], + "name": { + "given_name": "Christopher", + "middle_name": "J.", + "pubraw": "Christopher J. Wood", + "surname": "Wood" + } }, { "name": { - "surname": "Osvaldo Gonzalez Aceves", "given_name": "Blas", - "pubraw": "Blas Osvaldo Gonzalez Aceves" + "pubraw": "Blas Osvaldo Gonzalez Aceves", + "surname": "Osvaldo Gonzalez Aceves" } }, { - "name": { - "surname": "Rodriguez", - "given_name": "Baltazar", - "pubraw": "Baltazar Rodriguez" - }, "affiliation": [ { "affPubRaw": "IBM" } - ] + ], + "name": { + "given_name": "Baltazar", + "pubraw": "Baltazar Rodriguez", + "surname": "Rodriguez" + } }, { "name": { @@ -313,37 +280,70 @@ } }, { - "name": { - "surname": "Amano", - "given_name": "Takehiko" - }, "affiliation": [ { "affPubRaw": "IBM" } - ] + ], + "name": { + "given_name": "Takehiko", + "surname": "Amano" + } }, { - "name": { - "surname": "Pozas-Kerstjens", - "given_name": "Alex", - "pubraw": "Alex Pozas-Kerstjens" - }, "affiliation": [ { "affPubRaw": "ICFO" } - ] + ], + "name": { + "given_name": "Alex", + "pubraw": "Alex Pozas-Kerstjens", + "surname": "Pozas-Kerstjens" + } } ], - "title": { - "textEnglish": "Qiskit/qiskit: Qiskit 0.12.1" - }, - "abstract": { - "textEnglish": "Changed Increased the qiskit-ibmq-provider version to the latest release 0.3.3." - }, "doctype": "software", "openAccess": { "open": true + }, + "persistentIDs": [ + { + "DOI": "10.5281/zenodo.3465853" + } + ], + "pubDate": { + "electrDate": "2019", + "otherDate": [ + { + "otherDateType": "Issued", + "otherDateValue": "2019-09-30" + } + ] + }, + "publication": { + "pubYear": "2019", + "publisher": "Zenodo" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "relatedTo": [ + { + "relatedDocID": "https://github.com/Qiskit/qiskit/tree/0.12.1", + "relationship": "supplement" + }, + { + "relatedDocID": "10.5281/zenodo.2573505", + "relationship": "related" + } + ], + "title": { + "textEnglish": "Qiskit/qiskit: Qiskit 0.12.1" } } diff --git a/tests/stubdata/output/zenodo_test3.json b/tests/stubdata/output/zenodo_test3.json index 660f1f4..88663b7 100644 --- a/tests/stubdata/output/zenodo_test3.json +++ b/tests/stubdata/output/zenodo_test3.json @@ -1,71 +1,38 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" - }, - "relatedTo": [ - { - "relationship": "supplement", - "relatedDocID": "https://github.com/tqdm/tqdm/tree/v4.18.0" - }, - { - "relationship": "related", - "relatedDocID": "10.5281/zenodo.595120" - } - ], - "pubDate": { - "electrDate": "2017", - "otherDate": [ - { - "otherDateType": "Issued", - "otherDateValue": "2017-09-30" - } - ] - }, - "publication": { - "publisher": "Zenodo", - "pubYear": "2017" + "abstract": { + "textEnglish": "Thread safety! (#285 -> #291 -> #329, #407, #417) Ease redirection of sys.stdout/stderr (#422) Minor internal stream bugfix (#439) AttributeError fixes (#323, #324, #418) Related to: Misc bugs (#334) concurrent.futures (#97) Multi-tqdm (#143) flush() and refresh() (#331) Newline on refresh() (#361) Nested trees (#384) Manually positioned nested bars clearing (#385)" }, - "persistentIDs": [ - { - "DOI": "10.5281/zenodo.1000003" - } - ], "authors": [ { "name": { - "surname": "da Costa-Luis", "given_name": "Casper", - "pubraw": "Casper da Costa-Luis" + "pubraw": "Casper da Costa-Luis", + "surname": "da Costa-Luis" } }, { - "name": { - "surname": "L.", - "given_name": "Stephen", - "pubraw": "Stephen L." - }, "affiliation": [ { "affPubRaw": "Coma Science Group" } - ] + ], + "name": { + "given_name": "Stephen", + "pubraw": "Stephen L.", + "surname": "L." + } }, { - "name": { - "surname": "Mary", - "given_name": "Hadrien", - "pubraw": "Hadrien Mary" - }, "affiliation": [ { "affPubRaw": "University of McGill" } - ] + ], + "name": { + "given_name": "Hadrien", + "pubraw": "Hadrien Mary", + "surname": "Mary" + } }, { "name": { @@ -74,22 +41,22 @@ } }, { - "name": { - "surname": "Korobov", - "given_name": "Mikhail", - "pubraw": "Mikhail Korobov" - }, "affiliation": [ { "affPubRaw": "@ScrapingHub" } - ] + ], + "name": { + "given_name": "Mikhail", + "pubraw": "Mikhail Korobov", + "surname": "Korobov" + } }, { "name": { - "surname": "Ivanov", "given_name": "Ivan", - "pubraw": "Ivan Ivanov" + "pubraw": "Ivan Ivanov", + "surname": "Ivanov" } }, { @@ -99,17 +66,17 @@ } }, { - "name": { - "surname": "Pagel", - "given_name": "Matthew", - "middle_name": "D.", - "pubraw": "Matthew D. Pagel" - }, "affiliation": [ { "affPubRaw": "UC Davis" } - ] + ], + "name": { + "given_name": "Matthew", + "middle_name": "D.", + "pubraw": "Matthew D. Pagel", + "surname": "Pagel" + } }, { "name": { @@ -118,42 +85,42 @@ } }, { - "name": { - "surname": "McCracken", - "given_name": "Jack", - "pubraw": "Jack McCracken" - }, "affiliation": [ { "affPubRaw": "@Shopify" } - ] + ], + "name": { + "given_name": "Jack", + "pubraw": "Jack McCracken", + "surname": "McCracken" + } }, { "name": { - "surname": "Dill", "given_name": "Fabian", - "pubraw": "Fabian Dill" + "pubraw": "Fabian Dill", + "surname": "Dill" } }, { "name": { - "surname": "Panteleit", "given_name": "Daniel", - "pubraw": "Daniel Panteleit" + "pubraw": "Daniel Panteleit", + "surname": "Panteleit" } }, { - "name": { - "surname": "Rothberg", - "given_name": "Alex", - "pubraw": "Alex Rothberg" - }, "affiliation": [ { "affPubRaw": "4Catalyzer" } - ] + ], + "name": { + "given_name": "Alex", + "pubraw": "Alex Rothberg", + "surname": "Rothberg" + } }, { "name": { @@ -162,16 +129,16 @@ } }, { - "name": { - "surname": "Coccioli", - "given_name": "Riccardo", - "pubraw": "Riccardo Coccioli" - }, "affiliation": [ { "affPubRaw": "Wikimedia Foundation" } - ] + ], + "name": { + "given_name": "Riccardo", + "pubraw": "Riccardo Coccioli", + "surname": "Coccioli" + } }, { "name": { @@ -187,40 +154,40 @@ }, { "name": { - "surname": "Kottke", "given_name": "Albert", - "pubraw": "Albert Kottke" + "pubraw": "Albert Kottke", + "surname": "Kottke" } }, { - "name": { - "surname": "Halchenko", - "given_name": "Yaroslav", - "pubraw": "Yaroslav Halchenko" - }, "affiliation": [ { "affPubRaw": "Dartmouth College, @Debian, @DataLad, @PyMVPA, @fail2ban" } - ] + ], + "name": { + "given_name": "Yaroslav", + "pubraw": "Yaroslav Halchenko", + "surname": "Halchenko" + } }, { - "name": { - "surname": "Ostasevicius", - "given_name": "Tomas", - "pubraw": "Tomas Ostasevicius" - }, "affiliation": [ { "affPubRaw": "University of Cambridge" } - ] + ], + "name": { + "given_name": "Tomas", + "pubraw": "Tomas Ostasevicius", + "surname": "Ostasevicius" + } }, { "name": { - "surname": "Pokharel", "given_name": "Shirish", - "pubraw": "Shirish Pokharel" + "pubraw": "Shirish Pokharel", + "surname": "Pokharel" } }, { @@ -231,16 +198,16 @@ }, { "name": { - "surname": "VandeHaar", "given_name": "Peter", - "pubraw": "Peter VandeHaar" + "pubraw": "Peter VandeHaar", + "surname": "VandeHaar" } }, { "name": { - "surname": "Wu", "given_name": "Kuang-che", - "pubraw": "Kuang-che Wu" + "pubraw": "Kuang-che Wu", + "surname": "Wu" } }, { @@ -250,33 +217,33 @@ } }, { - "name": { - "given_name": "Hugo", - "pubraw": "Hugo" - }, "affiliation": [ { "affPubRaw": "Nord Software" } - ] + ], + "name": { + "given_name": "Hugo", + "pubraw": "Hugo" + } }, { - "name": { - "surname": "Hurley", - "given_name": "Ford", - "pubraw": "Ford Hurley" - }, "affiliation": [ { "affPubRaw": "@handwritingio" } - ] + ], + "name": { + "given_name": "Ford", + "pubraw": "Ford Hurley", + "surname": "Hurley" + } }, { "name": { - "surname": "Persaud", "given_name": "Arun", - "pubraw": "Arun Persaud" + "pubraw": "Arun Persaud", + "surname": "Persaud" } }, { @@ -286,26 +253,59 @@ } }, { - "name": { - "surname": "Umer", - "given_name": "Adnan", - "pubraw": "Adnan Umer" - }, "affiliation": [ { "affPubRaw": "@arbisoft" } - ] + ], + "name": { + "given_name": "Adnan", + "pubraw": "Adnan Umer", + "surname": "Umer" + } } ], - "title": { - "textEnglish": "tqdm/tqdm: tqdm v4.18.0 stable" - }, - "abstract": { - "textEnglish": "Thread safety! (#285 -> #291 -> #329, #407, #417) Ease redirection of sys.stdout/stderr (#422) Minor internal stream bugfix (#439) AttributeError fixes (#323, #324, #418) Related to: Misc bugs (#334) concurrent.futures (#97) Multi-tqdm (#143) flush() and refresh() (#331) Newline on refresh() (#361) Nested trees (#384) Manually positioned nested bars clearing (#385)" - }, "doctype": "software", "openAccess": { "open": true + }, + "persistentIDs": [ + { + "DOI": "10.5281/zenodo.1000003" + } + ], + "pubDate": { + "electrDate": "2017", + "otherDate": [ + { + "otherDateType": "Issued", + "otherDateValue": "2017-09-30" + } + ] + }, + "publication": { + "pubYear": "2017", + "publisher": "Zenodo" + }, + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "relatedTo": [ + { + "relatedDocID": "https://github.com/tqdm/tqdm/tree/v4.18.0", + "relationship": "supplement" + }, + { + "relatedDocID": "10.5281/zenodo.595120", + "relationship": "related" + } + ], + "title": { + "textEnglish": "tqdm/tqdm: tqdm v4.18.0 stable" } } diff --git a/tests/stubdata/output/zenodo_test4.json b/tests/stubdata/output/zenodo_test4.json index 7b5587c..808590f 100644 --- a/tests/stubdata/output/zenodo_test4.json +++ b/tests/stubdata/output/zenodo_test4.json @@ -1,36 +1,59 @@ { - "recordData": { - "createdTime": "", - "parsedTime": "", - "loadType": "fromFile", - "loadFormat": "OtherXML", - "loadLocation": "", - "recordOrigin": "" + "abstract": { + "textEnglish": "The final release of the supporting data and scripts to reproduce the figures in O. Newton et al. (2023). This Letter appears in The Astrophysical Journal Letters. A full description of the files and data contained in this repository is provided in the README file. What's Changed Bump contourpy from 1.0.6 to 1.0.7 by @dependabot in https://github.com/Musical-Neutron/lg_field_udgs/pull/16 Bump h5py from 3.7.0 to 3.8.0 by @dependabot in https://github.com/Musical-Neutron/lg_field_udgs/pull/17 Bump fonttools from 4.38.0 to 4.39.2 by @dependabot in https://github.com/Musical-Neutron/lg_field_udgs/pull/18 Fixing matplotlib warnings raised when running fig_04_plot_luminosity_functions.py and fig_05_plot_mock_sdss_observations.py Adding ApJL DOIs to README Full Changelog: https://github.com/Musical-Neutron/lg_field_udgs/compare/v1.0...v1.1" }, - "relatedTo": [ + "authors": [ { - "relationship": "supplement", - "relatedDocID": "https://github.com/Musical-Neutron/lg_field_udgs/tree/v1.1" + "affiliation": [ + { + "affPubRaw": "Center for Theoretical Physics, Polish Academy of Sciences" + } + ], + "attrib": { + "orcid": "0000-0002-2769-9507" + }, + "name": { + "given_name": "Oliver", + "pubraw": "Oliver Newton", + "surname": "Newton" + } + } + ], + "doctype": "software", + "keywords": [ + { + "keyString": "Ultra-diffuse galaxies", + "keySystem": "datacite" }, { - "relationship": "supplement", - "relatedDocID": "10.48550/arXiv.2212.05066" + "keyString": "Milky Way", + "keySystem": "datacite" }, { - "relationship": "supplement", - "relatedDocID": "10.3847/2041-8213/acc2bb" + "keyString": "Andromeda", + "keySystem": "datacite" }, { - "relationship": "related", - "relatedDocID": "10.5281/zenodo.7729995" + "keyString": "Local Group", + "keySystem": "datacite" }, { - "relationship": "related", - "relatedDocID": "https://zenodo.org/communities/aas" + "keyString": "HESTIA", + "keySystem": "datacite" }, { - "relationship": "related", - "relatedDocID": "https://zenodo.org/communities/astronomy-general" + "keyString": "Python", + "keySystem": "datacite" + } + ], + "openAccess": { + "license": "GNU Affero General Public License v3.0", + "licenseURL": "https://opensource.org/licenses/AGPL-3.0", + "open": true + }, + "persistentIDs": [ + { + "DOI": "10.5281/zenodo.7757685" } ], "pubDate": { @@ -43,36 +66,16 @@ ] }, "publication": { - "publisher": "Zenodo", - "pubYear": "2023" - }, - "persistentIDs": [ - { - "DOI": "10.5281/zenodo.7757685" - } - ], - "authors": [ - { - "name": { - "surname": "Newton", - "given_name": "Oliver", - "pubraw": "Oliver Newton" - }, - "affiliation": [ - { - "affPubRaw": "Center for Theoretical Physics, Polish Academy of Sciences" - } - ], - "attrib": { - "orcid": "0000-0002-2769-9507" - } - } - ], - "title": { - "textEnglish": "HESTIA Local Group field UDG paper scripts & reduced data" + "pubYear": "2023", + "publisher": "Zenodo" }, - "abstract": { - "textEnglish": "The final release of the supporting data and scripts to reproduce the figures in O. Newton et al. (2023). This Letter appears in The Astrophysical Journal Letters. A full description of the files and data contained in this repository is provided in the README file. What's Changed Bump contourpy from 1.0.6 to 1.0.7 by @dependabot in https://github.com/Musical-Neutron/lg_field_udgs/pull/16 Bump h5py from 3.7.0 to 3.8.0 by @dependabot in https://github.com/Musical-Neutron/lg_field_udgs/pull/17 Bump fonttools from 4.38.0 to 4.39.2 by @dependabot in https://github.com/Musical-Neutron/lg_field_udgs/pull/18 Fixing matplotlib warnings raised when running fig_04_plot_luminosity_functions.py and fig_05_plot_mock_sdss_observations.py Adding ApJL DOIs to README Full Changelog: https://github.com/Musical-Neutron/lg_field_udgs/compare/v1.0...v1.1" + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" }, "references": [ "10.1093/mnras/staa375", @@ -80,36 +83,33 @@ "10.3847/1538-4357/ac91cb", "10.1086/589911" ], - "doctype": "software", - "keywords": [ + "relatedTo": [ { - "keyString": "Ultra-diffuse galaxies", - "keySystem": "datacite" + "relatedDocID": "https://github.com/Musical-Neutron/lg_field_udgs/tree/v1.1", + "relationship": "supplement" }, { - "keyString": "Milky Way", - "keySystem": "datacite" + "relatedDocID": "10.48550/arXiv.2212.05066", + "relationship": "supplement" }, { - "keyString": "Andromeda", - "keySystem": "datacite" + "relatedDocID": "10.3847/2041-8213/acc2bb", + "relationship": "supplement" }, { - "keyString": "Local Group", - "keySystem": "datacite" + "relatedDocID": "10.5281/zenodo.7729995", + "relationship": "related" }, { - "keyString": "HESTIA", - "keySystem": "datacite" + "relatedDocID": "https://zenodo.org/communities/aas", + "relationship": "related" }, { - "keyString": "Python", - "keySystem": "datacite" + "relatedDocID": "https://zenodo.org/communities/astronomy-general", + "relationship": "related" } ], - "openAccess": { - "open": true, - "license": "GNU Affero General Public License v3.0", - "licenseURL": "https://opensource.org/licenses/AGPL-3.0" + "title": { + "textEnglish": "HESTIA Local Group field UDG paper scripts & reduced data" } } From f7fa30a8f286ab1c136cb8acdcd15e4111ae4612 Mon Sep 17 00:00:00 2001 From: Matthew Templeton Date: Thu, 18 Apr 2024 13:07:23 -0400 Subject: [PATCH 03/10] Added more mathml tags, updated unit test output modified: adsingestp/parsers/base.py modified: tests/stubdata/output/els_detag_example_2.json modified: tests/stubdata/output/jats_springer_EPJC_s10052-023-11699-1.json modified: tests/stubdata/output/jats_springer_JHEP_JHEP07_2023_200.json modified: tests/stubdata/output/jats_springer_ZaMP_s00033-023-02064-z.json modified: tests/test_elsevier.py --- adsingestp/parsers/base.py | 10 ++++++++++ tests/stubdata/output/els_detag_example_2.json | 2 +- .../output/jats_springer_EPJC_s10052-023-11699-1.json | 2 +- .../output/jats_springer_JHEP_JHEP07_2023_200.json | 4 ++-- .../output/jats_springer_ZaMP_s00033-023-02064-z.json | 2 +- tests/test_elsevier.py | 9 --------- 6 files changed, 15 insertions(+), 14 deletions(-) diff --git a/adsingestp/parsers/base.py b/adsingestp/parsers/base.py index 5ad0252..790d963 100644 --- a/adsingestp/parsers/base.py +++ b/adsingestp/parsers/base.py @@ -489,7 +489,17 @@ class BaseBeautifulSoupParser(IngestBase): "mml:mn", "mml:annotation", "mml:msubsup", + "mml:msupsub", "mml:msup", + "mml:mfrac", + "mml:munderovers", + "mml:msqrt", + "mml:mmultiscripts", + "mml:prescripts", + "mml:mtext", + "mml:mfenced", + "mml:mstyle", + "mml:mspace", ] HTML_TAGS_HTML = ["sub", "sup", "a", "astrobj", "i", "b"] diff --git a/tests/stubdata/output/els_detag_example_2.json b/tests/stubdata/output/els_detag_example_2.json index 09b8b39..b390f04 100644 --- a/tests/stubdata/output/els_detag_example_2.json +++ b/tests/stubdata/output/els_detag_example_2.json @@ -1,6 +1,6 @@ { "abstract": { - "textEnglish": "In this article, Hard-Wall AdS/QCD with 5 flavors is used to study pseudoscalar, vector and axial-vector B meson. The mass and decay constants of B0, Bs0, Bc\u2212, \u03b7b, Bs\u204e0, Bc\u204e\u2212, B1\u2212, B1s0, B1c\u2212, \u03b7b and \u03c7b1 as well as strong couplings of (B\u00af\u204e0,B\u204e+,\u03c0\u2212)(B\u204e+,Bs\u204e0,K+), (B\u00af10,B\u204e+,\u03c0\u2212), (B1\u204e+,Bs\u204e0,K+), (B\u00af10,B1+,\u03c1\u2212), (B\u00af1+,Bs10,K\u204e+), (B\u00af10,B\u204e+,a0\u2212), (B\u00af1+,Bs\u204e0,K0+), (D\u00af\u204e0,D\u204e\u2212,\u03c0\u2212), (D\u00af\u204e0,Ds\u204e\u2212,K+)(D\u00af\u204e0,D1\u2212,\u03c0\u2212), (D\u00af\u204e0,Ds1\u2212,K+), (D\u00af10,D1\u2212,\u03c1\u2212), (D\u00af10,Ds1\u2212,K\u204e+), (D\u00af\u204e0,D1\u2212,a0\u2212) and (D\u00af\u204e0,Ds1\u2212,K0+) vertices are estimated in this study. A comparison of the results of the masses, decay constants, and strong couplings with existing predictions is also made." + "textEnglish": "In this article, Hard-Wall AdS/QCD with 5 flavors is used to study pseudoscalar, vector and axial-vector B meson. The mass and decay constants of B0, Bs0, Bc\u2212, \u03b7b, Bs\u204e0, Bc\u204e\u2212, B1\u2212, B1s0, B1c\u2212, \u03b7b and \u03c7b1 as well as strong couplings of (B\u00af\u204e0,B\u204e+,\u03c0\u2212)(B\u204e+,Bs\u204e0,K+), (B\u00af10,B\u204e+,\u03c0\u2212), (B1\u204e+,Bs\u204e0,K+), (B\u00af10,B1+,\u03c1\u2212), (B\u00af1+,Bs10,K\u204e+), (B\u00af10,B\u204e+,a0\u2212), (B\u00af1+,Bs\u204e0,K0+), (D\u00af\u204e0,D\u204e\u2212,\u03c0\u2212), (D\u00af\u204e0,Ds\u204e\u2212,K+)(D\u00af\u204e0,D1\u2212,\u03c0\u2212), (D\u00af\u204e0,Ds1\u2212,K+), (D\u00af10,D1\u2212,\u03c1\u2212), (D\u00af10,Ds1\u2212,K\u204e+), (D\u00af\u204e0,D1\u2212,a0\u2212) and (D\u00af\u204e0,Ds1\u2212,K0+) vertices are estimated in this study. A comparison of the results of the masses, decay constants, and strong couplings with existing predictions is also made." }, "authors": [ { diff --git a/tests/stubdata/output/jats_springer_EPJC_s10052-023-11699-1.json b/tests/stubdata/output/jats_springer_EPJC_s10052-023-11699-1.json index f7b7df9..ac73e8d 100644 --- a/tests/stubdata/output/jats_springer_EPJC_s10052-023-11699-1.json +++ b/tests/stubdata/output/jats_springer_EPJC_s10052-023-11699-1.json @@ -1,6 +1,6 @@ { "abstract": { - "textEnglish": "The flavour-tagging algorithms developed by the ATLAS Collaboration and used to analyse its dataset of s = 13 \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$\\sqrt{s} = 13$$\\end{document} TeV pp collisions from Run 2 of the Large Hadron Collider are presented. These new tagging algorithms are based on recurrent and deep neural networks, and their performance is evaluated in simulated collision events. These developments yield considerable improvements over previous jet-flavour identification strategies. At the 77% b-jet identification efficiency operating point, light-jet (charm-jet) rejection factors of 170 (5) are achieved in a sample of simulated Standard Model t t \u00af \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$t\\bar{t}$$\\end{document} events; similarly, at a c-jet identification efficiency of 30%, a light-jet ( b-jet) rejection factor of 70 (9) is obtained." + "textEnglish": "The flavour-tagging algorithms developed by the ATLAS Collaboration and used to analyse its dataset of s = 13 \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$\\sqrt{s} = 13$$\\end{document} TeV pp collisions from Run 2 of the Large Hadron Collider are presented. These new tagging algorithms are based on recurrent and deep neural networks, and their performance is evaluated in simulated collision events. These developments yield considerable improvements over previous jet-flavour identification strategies. At the 77% b-jet identification efficiency operating point, light-jet (charm-jet) rejection factors of 170 (5) are achieved in a sample of simulated Standard Model t t \u00af \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$t\\bar{t}$$\\end{document} events; similarly, at a c-jet identification efficiency of 30%, a light-jet ( b-jet) rejection factor of 70 (9) is obtained." }, "authors": [ { diff --git a/tests/stubdata/output/jats_springer_JHEP_JHEP07_2023_200.json b/tests/stubdata/output/jats_springer_JHEP_JHEP07_2023_200.json index 0988301..5fda103 100644 --- a/tests/stubdata/output/jats_springer_JHEP_JHEP07_2023_200.json +++ b/tests/stubdata/output/jats_springer_JHEP_JHEP07_2023_200.json @@ -1,6 +1,6 @@ { "abstract": { - "textEnglish": "This article reports measurements of the angle between differently defined jet axes in pp collisions at s \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ \\sqrt{s} $$\\end{document} = 5 .02 TeV carried out by the ALICE Collaboration. Charged particles at midrapidity are clustered into jets with resolution parameters R = 0 .2 and 0.4. The jet axis, before and after Soft Drop grooming, is compared to the jet axis from the Winner-Takes-All (WTA) recombination scheme. The angle between these axes, \u2206 R axis, probes a wide phase space of the jet formation and evolution, ranging from the initial high-momentum-transfer scattering to the hadronization process. The \u2206 R axis observable is presented for 20 < p T ch jet \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ {p}_{\\textrm{T}}^{\\textrm{ch}\\ \\textrm{jet}} $$\\end{document} < 100 GeV/ c, and compared to predictions from the PYTHIA 8 and Herwig 7 event generators. The distributions can also be calculated analytically with a leading hadronization correction related to the non-perturbative component of the Collins-Soper-Sterman (CSS) evolution kernel. Comparisons to analytical predictions at next-to-leading-logarithmic accuracy with leading hadronization correction implemented from experimental extractions of the CSS kernel in Drell-Yan measurements are presented. The analytical predictions describe the measured data within 20% in the perturbative regime, with surprising agreement in the non-perturbative regime as well. These results are compatible with the universality of the CSS kernel in the context of jet substructure.\n" + "textEnglish": "This article reports measurements of the angle between differently defined jet axes in pp collisions at s \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ \\sqrt{s} $$\\end{document} = 5 .02 TeV carried out by the ALICE Collaboration. Charged particles at midrapidity are clustered into jets with resolution parameters R = 0 .2 and 0.4. The jet axis, before and after Soft Drop grooming, is compared to the jet axis from the Winner-Takes-All (WTA) recombination scheme. The angle between these axes, \u2206 R axis, probes a wide phase space of the jet formation and evolution, ranging from the initial high-momentum-transfer scattering to the hadronization process. The \u2206 R axis observable is presented for 20 < p T ch jet \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ {p}_{\\textrm{T}}^{\\textrm{ch}\\ \\textrm{jet}} $$\\end{document} < 100 GeV/ c, and compared to predictions from the PYTHIA 8 and Herwig 7 event generators. The distributions can also be calculated analytically with a leading hadronization correction related to the non-perturbative component of the Collins-Soper-Sterman (CSS) evolution kernel. Comparisons to analytical predictions at next-to-leading-logarithmic accuracy with leading hadronization correction implemented from experimental extractions of the CSS kernel in Drell-Yan measurements are presented. The analytical predictions describe the measured data within 20% in the perturbative regime, with surprising agreement in the non-perturbative regime as well. These results are compatible with the universality of the CSS kernel in the context of jet substructure.\n" }, "authors": [ { @@ -12254,6 +12254,6 @@ " Gieseke S Rohr C Siodmok A Colour reconnections in Herwig++ Eur. Phys. J. C 2012 72 2225 2012EPJC...72.2225G 10.1140/epjc/s10052-012-2225-5 [arXiv:1206.0041] [INSPIRE] " ], "title": { - "textEnglish": "Measurement of the angle between jet axes in pp collisions at s \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ \\sqrt{s} $$\\end{document} = 5 .02 TeV" + "textEnglish": "Measurement of the angle between jet axes in pp collisions at s \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ \\sqrt{s} $$\\end{document} = 5 .02 TeV" } } diff --git a/tests/stubdata/output/jats_springer_ZaMP_s00033-023-02064-z.json b/tests/stubdata/output/jats_springer_ZaMP_s00033-023-02064-z.json index 6847da0..663def7 100644 --- a/tests/stubdata/output/jats_springer_ZaMP_s00033-023-02064-z.json +++ b/tests/stubdata/output/jats_springer_ZaMP_s00033-023-02064-z.json @@ -1,6 +1,6 @@ { "abstract": { - "textEnglish": "This paper is concerned with the time-asymptotic stability of a nonlinear wave for the outflow problem of the isentropic compressible Navier\u2013Stokes\u2013Korteweg equations in the half space. Under some suitable assumptions on the spatial-asymptotic states and boundary data, the time-asymptotic profile is a nonlinear wave which is the superposition of a stationary solution and a rarefaction wave. Employing the L 2 \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$L^{2}$$\\end{document} -energy method and the decay (in both time and space variables) estimates of each component of the nonlinear wave, we prove that this nonlinear wave is time asymptotically stable under a small initial perturbation." + "textEnglish": "This paper is concerned with the time-asymptotic stability of a nonlinear wave for the outflow problem of the isentropic compressible Navier\u2013Stokes\u2013Korteweg equations in the half space. Under some suitable assumptions on the spatial-asymptotic states and boundary data, the time-asymptotic profile is a nonlinear wave which is the superposition of a stationary solution and a rarefaction wave. Employing the L 2 \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$L^{2}$$\\end{document} -energy method and the decay (in both time and space variables) estimates of each component of the nonlinear wave, we prove that this nonlinear wave is time asymptotically stable under a small initial perturbation." }, "authors": [ { diff --git a/tests/test_elsevier.py b/tests/test_elsevier.py index 6c47536..d224fab 100644 --- a/tests/test_elsevier.py +++ b/tests/test_elsevier.py @@ -7,15 +7,6 @@ from adsingestp.parsers import elsevier -# import logging -# proj_dir = os.path.abspath(os.path.join(os.path.dirname(__file__), os.pardir, "adsingestp")) -# logging.basicConfig( -# format="%(levelname)s %(asctime)s %(message)s", -# filename=os.path.join(proj_dir, "logs", "parser.log"), -# level=logging.INFO, -# force=True, -# ) - TIMESTAMP_FMT = "%Y-%m-%dT%H:%M:%S.%fZ" From 03fb9ba406ea78fd36b330bafda95051387dff4d Mon Sep 17 00:00:00 2001 From: Matthew Templeton Date: Thu, 18 Apr 2024 16:16:51 -0400 Subject: [PATCH 04/10] Adding untested cases to tests with stubdata new file: tests/stubdata/output/jats_aps_phrvd_100_052015.json new file: tests/stubdata/output/jats_aps_phrvx_12_021031.json new file: tests/stubdata/output/jats_edp_aa_661_70.json new file: tests/stubdata/output/jats_edp_jnwpu_40_96.json new file: tests/stubdata/output/jats_iop_jinst_17_05_P05009.json new file: tests/stubdata/output/jats_nature_natsd_12_7375.json new file: tests/stubdata/output/jats_pnas_119_2201344119.json new file: tests/stubdata/output/jats_springer_cldy_84_1543.json new file: tests/stubdata/output/jats_springer_jhep_2022_05_05.json new file: tests/stubdata/output/mdpi_climate-11-00147.json new file: tests/stubdata/output/mdpi_galaxies-11-00090.json new file: tests/stubdata/output/mdpi_symmetry-15-00939.json new file: tests/stubdata/output/mdpi_universe-08-00651.json new file: tests/stubdata/output/nlm_tf_gapfd_116_38.json modified: tests/test_elsevier.py modified: tests/test_jats.py --- .../output/jats_aps_phrvd_100_052015.json | 6687 +++ .../output/jats_aps_phrvx_12_021031.json | 166 + tests/stubdata/output/jats_edp_aa_661_70.json | 190 + .../stubdata/output/jats_edp_jnwpu_40_96.json | 231 + .../output/jats_iop_jinst_17_05_P05009.json | 10468 +++++ .../output/jats_nature_natsd_12_7375.json | 1513 + .../output/jats_pnas_119_2201344119.json | 71 + .../output/jats_springer_cldy_84_1543.json | 363 + .../output/jats_springer_jhep_2022_05_05.json | 33607 ++++++++++++++++ .../output/mdpi_climate-11-00147.json | 289 + .../output/mdpi_galaxies-11-00090.json | 240 + .../output/mdpi_symmetry-15-00939.json | 231 + .../output/mdpi_universe-08-00651.json | 270 + .../stubdata/output/nlm_tf_gapfd_116_38.json | 178 + tests/test_elsevier.py | 3 +- tests/test_jats.py | 16 +- 16 files changed, 54519 insertions(+), 4 deletions(-) create mode 100644 tests/stubdata/output/jats_aps_phrvd_100_052015.json create mode 100644 tests/stubdata/output/jats_aps_phrvx_12_021031.json create mode 100644 tests/stubdata/output/jats_edp_aa_661_70.json create mode 100644 tests/stubdata/output/jats_edp_jnwpu_40_96.json create mode 100644 tests/stubdata/output/jats_iop_jinst_17_05_P05009.json create mode 100644 tests/stubdata/output/jats_nature_natsd_12_7375.json create mode 100644 tests/stubdata/output/jats_pnas_119_2201344119.json create mode 100644 tests/stubdata/output/jats_springer_cldy_84_1543.json create mode 100644 tests/stubdata/output/jats_springer_jhep_2022_05_05.json create mode 100644 tests/stubdata/output/mdpi_climate-11-00147.json create mode 100644 tests/stubdata/output/mdpi_galaxies-11-00090.json create mode 100644 tests/stubdata/output/mdpi_symmetry-15-00939.json create mode 100644 tests/stubdata/output/mdpi_universe-08-00651.json create mode 100644 tests/stubdata/output/nlm_tf_gapfd_116_38.json diff --git a/tests/stubdata/output/jats_aps_phrvd_100_052015.json b/tests/stubdata/output/jats_aps_phrvd_100_052015.json new file mode 100644 index 0000000..1a432af --- /dev/null +++ b/tests/stubdata/output/jats_aps_phrvd_100_052015.json @@ -0,0 +1,6687 @@ +{ + "abstract": { + "textEnglish": "Using a data sample of 1.31\u00d7109 J/\u03c8 events collected with the BESIII detector, a search for \u03b7\u2032\u2192\u03b3\u03b3\u03b7 via J/\u03c8\u2192\u03b3\u03b7\u2032 is performed for the first time. No significant \u03b7\u2032 signal is observed in the \u03b3\u03b3\u03b7 invariant mass spectrum, and the branching fraction of \u03b7\u2032\u2192\u03b3\u03b3\u03b7 is determined to be less than 1.33\u00d710-4 at the 90% confidence level." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "a1", + "affPubRaw": "Institute of High Energy Physics, Beijing 100049, People\u2019s Republic of China" + } + ], + "name": { + "given_name": "M.", + "surname": "Ablikim" + } + }, + { + "affiliation": [ + { + "affPubID": "a10", + "affPubRaw": "G.I. Budker Institute of Nuclear Physics SB RAS (BINP), Novosibirsk 630090, Russia" + } + ], + "name": { + "given_name": "M.\u2009N.", + "surname": "Achasov" + } + }, + { + "affiliation": [ + { + "affPubID": "a59", + "affPubRaw": "Uppsala University, Box 516, SE-75120 Uppsala, Sweden" + } + ], + "name": { + "given_name": "P.", + "surname": "Adlarson" + } + }, + { + "affiliation": [ + { + "affPubID": "a15", + "affPubRaw": "Helmholtz Institute Mainz, Johann-Joachim-Becher-Weg 45, D-55099 Mainz, Germany" + } + ], + "name": { + "given_name": "S.", + "surname": "Ahmed" + } + }, + { + "affiliation": [ + { + "affPubID": "a4", + "affPubRaw": "Bochum Ruhr-University, D-44780 Bochum, Germany" + } + ], + "name": { + "given_name": "M.", + "surname": "Albrecht" + } + }, + { + "affiliation": [ + { + "affPubID": "a58a", + "affPubRaw": "University of Turin, I-10125 Turin, Italy" + }, + { + "affPubID": "a58c", + "affPubRaw": "INFN, I-10125 Turin, Italy" + } + ], + "name": { + "given_name": "M.", + "surname": "Alekseev" + } + }, + { + "affiliation": [ + { + "affPubID": "a58a", + "affPubRaw": "University of Turin, I-10125 Turin, Italy" + }, + { + "affPubID": "a58c", + "affPubRaw": "INFN, I-10125 Turin, Italy" + } + ], + "name": { + "given_name": "A.", + "surname": "Amoroso" + } + }, + { + "affiliation": [ + { + "affPubID": "a1", + "affPubRaw": "Institute of High Energy Physics, Beijing 100049, People\u2019s Republic of China" + } + ], + "name": { + "given_name": "F.\u2009F.", + "surname": "An" + } + }, + { + "affiliation": [ + { + "affPubID": "a55", + "affPubRaw": "University of Science and Technology of China, Hefei 230026, People\u2019s Republic of China" + }, + { + "affPubID": "a43", + "affPubRaw": "State Key Laboratory of Particle Detection and Electronics, Beijing 100049, Hefei 230026, People\u2019s Republic of China" + } + ], + "name": { + "given_name": "Q.", + "surname": "An" + } + }, + { + "affiliation": [ + { + "affPubID": "a42", + "affPubRaw": "Southeast University, Nanjing 211100, People\u2019s Republic of China" + } + ], + "name": { + "given_name": "Y.", + "surname": "Bai" + } + }, + { + "affiliation": [ + { + "affPubID": "a27", + "affPubRaw": "Joint Institute for Nuclear Research, 141980 Dubna, Moscow region, Russia" + } + ], + "name": { + "given_name": "O.", + "surname": "Bakina" + } + }, + { + "affiliation": [ + { + "affPubID": "a23a", + "affPubRaw": "INFN Laboratori Nazionali di Frascati, I-00044 Frascati, Italy" + } + ], + "name": { + "given_name": "R. 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C 41, 013001 (2017).CPCHCQ1674-113710.1088/1674-1137/41/1/013001" + ], + "title": { + "textEnglish": "Search for the decay \u03b7\u2032\u2192\u03b3\u03b3\u03b7" + } +} diff --git a/tests/stubdata/output/jats_aps_phrvx_12_021031.json b/tests/stubdata/output/jats_aps_phrvx_12_021031.json new file mode 100644 index 0000000..641ce34 --- /dev/null +++ b/tests/stubdata/output/jats_aps_phrvx_12_021031.json @@ -0,0 +1,166 @@ +{ + "abstract": { + "textEnglish": "A general mechanism is presented by which topological physics arises in strongly correlated systems without flat bands. Starting from a charge transfer insulator, topology emerges when the charge transfer energy between the cation and anion is reduced to invert the lower Hubbard band and the spin-degenerate charge transfer band. A universal low-energy theory is developed for the inversion of the charge transfer gap in a quantum antiferromagnet. The inverted state is found to be a quantum anomalous Hall (QAH) insulator with noncoplanar magnetism. Interactions play two essential roles in this mechanism: producing the insulating gap and quasiparticle bands prior to the band inversion, and causing the change of magnetic order necessary for the QAH effect after inversion. Our theory explains the electric-field-induced transition from a correlated insulator to a QAH state in AB-stacked transition-metal-dichalcogenides bilayer MoTe2/WSe2." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "a1", + "affPubRaw": "Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA" + } + ], + "attrib": { + "orcid": "0000-0002-4129-897X" + }, + "name": { + "given_name": "Trithep", + "surname": "Devakul" + } + }, + { + "affiliation": [ + { + "affPubID": "a1", + "affPubRaw": "Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA" + } + ], + "name": { + "given_name": "Liang", + "surname": "Fu" + } + } + ], + "copyright": { + "statement": "Published by the American Physical Society", + "status": true + }, + "funding": [ + { + "agencyid": { + "idschema": "doi", + "idvalue": "10.13039/100000893" + }, + "agencyname": "Simons Foundation" + }, + { + "agencyid": { + "idschema": "doi", + "idvalue": "10.13039/100000015" + }, + "agencyname": "U.S. Department of Energy", + "awardnumber": "DE-SC0020149" + }, + { + "agencyid": { + "idschema": "doi", + "idvalue": "10.13039/100000008" + }, + "agencyname": "David and Lucile Packard Foundation" + } + ], + "openAccess": { + "license": "Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article\u2019s title, journal citation, and DOI.", + "licenseURL": "https://creativecommons.org/licenses/by/4.0/" + }, + "pagination": { + "electronicID": "021031", + "pageCount": "14" + }, + "persistentIDs": [ + { + "DOI": "10.1103/PhysRevX.12.021031" + } + ], + "pubDate": { + "electrDate": "2022-05-06", + "printDate": "2022-04-01" + }, + "publication": { + "ISSN": [ + { + "issnString": "2160-3308", + "pubtype": "epub" + } + ], + "issueNum": "2", + "pubName": "Physical Review X", + "pubYear": "2022", + "publisher": "American Physical Society", + "volumeNum": "12" + }, + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + "1N.\u2009F. Mott, The Basis of the Electron Theory of Metals, with Special Reference to the Transition Metals, Proc. Phys. Soc. London Sect. 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I study how this information varies as a function of the scale cut applied, either with angular cut \u2113max or physical cut kmax. For this, I use analytical covariances with the most complete census of non-Gaussian terms, which proves to be critical. I find that the Fisher information on most cosmological and astrophysical parameters shows a striking behaviour. Beyond the perturbative regime, we first get decreasing returns: the information continues to rise but the slope slows down until reaching saturation. The location of this plateau, at k \u223c 2 Mpc\u22121, is slightly beyond the reach of current modelling methods and depends to some extent on the parameter and redshift bin considered. I explain the origin of this plateau, which is due to non-linear effects both on the power spectrum, and more importantly on non-Gaussian covariance terms. Then, pushing further, we see the information rising again in the highly non-linear regime, with a steep slope. This is the small-scale miracle, for which I give my interpretation and discuss the properties. There are suggestions that it may be possible to disentangle this information from the astrophysical content, and improve dark energy constraints. Finally, more hints are shown that high-order statistics may yield significant improvements over the power spectrum in this regime, with the improvements increasing with kmax. \u22c6 Data and notebooks reproducing all plots and results are available at https://github.com/fabienlacasa/SmallScaleMiracle" + }, + "authors": [ + { + "affiliation": [ + { + "affPubRaw": "Institut d\u2019Astrophysique Spatiale (IAS) , B\u00e2timent 121 , 91405 Orsay , France" + }, + { + "affPubRaw": "Universit\u00e9 Paris-Sud 11 and CNRS, UMR 8617 , France" + }, + { + "affPubRaw": "D\u00e9partement de Physique Th\u00e9orique and Center for Astroparticle Physics, Universit\u00e9 de Gen\u00e8ve , 24 quai Ernest Ansermet , 1211 Geneva , Switzerland" + } + ], + "attrib": { + "orcid": "0000-0002-7268-3440" + }, + "name": { + "given_name": "Fabien", + "surname": "Lacasa" + } + } + ], + "copyright": { + "statement": "\u00a9 F. Lacasa 2022", + "status": true + }, + "editorialHistory": { + "acceptedDate": "2022-03-11", + "receivedDates": [ + "2020-01-15" + ] + }, + "esources": [ + { + "location": "https://www.aanda.org/articles/aa/full_html/2022/05/aa37512-20/aa37512-20.html", + "source": "pub_html" + }, + { + "location": "https://www.aanda.org/articles/aa/pdf/2022/05/aa37512-20.pdf", + "source": "pub_pdf" + } + ], + "funding": [ + { + "agencyid": { + "idvalue": "Swiss National Science Foundation (SNSF)" + }, + "awardnumber": "IZSEZ0_207059" + } + ], + "keywords": [ + { + "keyString": "large-scale structure of Universe", + "keySystem": "misc" + }, + { + "keyString": "galaxies: statistics", + "keySystem": "misc" + } + ], + "openAccess": { + "license": "Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.", + "licenseURL": "https://www.edpsciences.org", + "open": true + }, + "pagination": { + "electronicID": "A70", + "pageCount": "12" + }, + "persistentIDs": [ + { + "DOI": "10.1051/0004-6361/202037512" + } + ], + "pubDate": { + "electrDate": "2022-05-02", + "printDate": "2022-05-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "0004-6361", + "pubtype": "ppub" + }, + { + "issnString": "1432-0746", + "pubtype": "epub" + } + ], + "issueNum": "None", + "pubName": "Astronomy & Astrophysics", + "pubYear": "2022", + "publisher": "EDP Sciences", + "volumeNum": "661" + }, + "publisherIDs": [ + { + "Identifier": "aa37512-20", + "attribute": "publisher-id" + }, + { + "Identifier": "2022A%26A...661A..70L", + "attribute": "other" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + " Abadi, M. 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C. 2008, ApJ, 676, 248 ", + " Zehavi, I., Zheng, Z., Weinberg, D. H., et al. 2011, ApJ, 736, 59 " + ], + "title": { + "textEnglish": "Cosmology in the non-linear regime: the small scale miracle", + "textNotes": [ + "\u22c6 Data and notebooks reproducing all plots and results are available at https://github.com/fabienlacasa/SmallScaleMiracle" + ] + } +} diff --git a/tests/stubdata/output/jats_edp_jnwpu_40_96.json b/tests/stubdata/output/jats_edp_jnwpu_40_96.json new file mode 100644 index 0000000..c4d36cf --- /dev/null +++ b/tests/stubdata/output/jats_edp_jnwpu_40_96.json @@ -0,0 +1,231 @@ +{ + "abstract": { + "textEnglish": "With the aging of the population, the decline of human body function leads to the decline of limb flexibility, and the severe cases lose the ability to walk. Research shows that the lower limb exoskeleton can assist human walking. In this paper, a lower limb exoskeleton is designed, which can collect the energy of the healthy side of the lower limb and release it when the affected side of the lower limb walks. The unilateral lower limb is used to compensate the movement of the affected limb, assist walking, and realize the collection, management and migration of human motion energy. The results showed that the root mean square value of rectus femoris decreased by 10%, and the EMG integral value of lateral gastrocnemius muscle decreased by 12%. The effect of exoskeleton on lower limb muscles is obvious. The walking assisted exoskeleton can provide auxiliary tension for lower limb movement and reduce muscle activity." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "AFF1", + "affPubRaw": "Shaanxi Engineering Laboratory for Transmissions and Controls, Northwestern Polytechnical University, Xi'an 710072, China" + }, + { + "affPubID": "AFF2", + "affPubRaw": "Xi'an Aeronautical University, Xi'an 710077, China" + } + ], + "attrib": { + "email": "zhou-xin@mail.nwpu.edu.cn" + }, + "name": { + "given_name": "Xin", + "surname": "ZHOU" + } + }, + { + "affiliation": [ + { + "affPubID": "AFF1", + "affPubRaw": "Shaanxi Engineering Laboratory for Transmissions and Controls, Northwestern Polytechnical University, Xi'an 710072, China" + } + ], + "name": { + "given_name": "Geng", + "surname": "LIU" + } + }, + { + "affiliation": [ + { + "affPubID": "AFF3", + "affPubRaw": "College of Art and Design, Shaanxi University of Science and Technology, Xi'an 710021, China" + } + ], + "name": { + "given_name": "Yunqi", + "surname": "TANG" + } + }, + { + "affiliation": [ + { + "affPubID": "AFF1", + "affPubRaw": "Shaanxi Engineering Laboratory for Transmissions and Controls, Northwestern Polytechnical University, Xi'an 710072, China" + } + ], + "name": { + "given_name": "Bing", + "surname": "HAN" + } + }, + { + "affiliation": [ + { + "affPubID": "AFF4", + "affPubRaw": "Xi'an Children's Hospital, Xi'an 710003, China" + } + ], + "name": { + "given_name": "Xiaoli", + "surname": "LIU" + } + } + ], + "copyright": { + "statement": "\u00a9 2022 Journal of Northwestern Polytechnical University. All rights reserved.", + "status": true + }, + "editorialHistory": { + "receivedDates": [ + "2021-06-07" + ] + }, + "esources": [ + { + "location": "https://www.jnwpu.org/articles/jnwpu/full_html/2022/01/jnwpu2022401p95/jnwpu2022401p95.html", + "source": "pub_html" + }, + { + "location": "https://www.jnwpu.org/articles/jnwpu/pdf/2022/01/jnwpu2022401p95.pdf", + "source": "pub_pdf" + } + ], + "funding": [ + { + "agencyname": "\u4e2d\u592e\u9ad8\u6821\u57fa\u7840\u7814\u7a76\u57fa\u91d1", + "awardnumber": "31020190503004" + }, + { + "agencyname": "\u9ad8\u7b49\u5b66\u6821\u5b66\u79d1\u521b\u65b0\u5f15\u667a\u8ba1\u5212", + "awardnumber": "B13044" + }, + { + "agencyname": "\u897f\u5b89\u5e02\u513f\u7ae5\u533b\u9662\u9879\u76ee", + "awardnumber": "2020D06" + } + ], + "keywords": [ + { + "keyString": "exoskeleton", + "keySystem": "misc" + }, + { + "keyString": "human energy", + "keySystem": "misc" + }, + { + "keyString": "energy harvester", + "keySystem": "misc" + }, + { + "keyString": "assist movement", + "keySystem": "misc" + }, + { + "keyString": "energy transfer", + "keySystem": "misc" + }, + { + "keyString": "\u5916\u9aa8\u9abc", + "keySystem": "misc" + }, + { + "keyString": "\u4eba\u4f53\u80fd\u91cf", + "keySystem": "misc" + }, + { + "keyString": "\u80fd\u91cf\u6536\u96c6\u5668", + "keySystem": "misc" + }, + { + "keyString": "\u8f85\u52a9\u8fd0\u52a8", + "keySystem": "misc" + }, + { + "keyString": "\u80fd\u91cf\u8fc1\u79fb", + "keySystem": "misc" + } + ], + "openAccess": { + "license": "This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.", + "licenseURL": "http://creativecommons.org/licenses/by/4.0", + "open": true + }, + "pagination": { + "firstPage": "95", + "lastPage": "102", + "pageCount": "8", + "pageRange": "95-102" + }, + "persistentIDs": [ + { + "DOI": "10.1051/jnwpu/20224010095" + } + ], + "pubDate": { + "electrDate": "2022-05-02", + "printDate": "2022-02-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "1000-2758", + "pubtype": "ppub" + }, + { + "issnString": "2609-7125", + "pubtype": "epub" + } + ], + "issueNum": "1", + "pubName": "Xibei Gongye Daxue Xuebao/Journal of Northwestern Polytechnical University", + "pubYear": "2022", + "publisher": "The Northwestern Polytechnical University", + "volumeNum": "40" + }, + "publisherIDs": [ + { + "Identifier": "jnwpu2022401p95", + "attribute": "publisher-id" + }, + { + "Identifier": "TH122", + "attribute": "other" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + "Jia Jianping. 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Chinese Journal of physical medicine and rehabilitation, 2003 (4): 22\u201325[Article] (in Chinese)" + ], + "title": { + "textEnglish": "Analysis and evaluation of human lower limb energy collection and walking assisted exoskeleton" + } +} diff --git a/tests/stubdata/output/jats_iop_jinst_17_05_P05009.json b/tests/stubdata/output/jats_iop_jinst_17_05_P05009.json new file mode 100644 index 0000000..d99fa4a --- /dev/null +++ b/tests/stubdata/output/jats_iop_jinst_17_05_P05009.json @@ -0,0 +1,10468 @@ +{ + "abstract": { + "textEnglish": "The centrality of heavy-ion collisions is directly related to the created medium in these interactions. A procedure to determine the centrality of collisions with the LHCb detector is implemented for lead-lead collisions at \u221as NN = 5 TeV and lead-neon fixed-target collisions at \u221as NN = 69 GeV. The energy deposits in the electromagnetic calorimeter are used to determine and define the centrality classes. The correspondence between the number of participants and the centrality for the lead-lead collisions is in good agreement with the correspondence found in other experiments, and the centrality measurements for the lead-neon collisions presented here are performed for the first time in fixed-target collisions at the LHC." + }, + "authors": [ + { + "attrib": { + "collab": true + }, + "name": { + "collab": "The LHCb collaboration" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation32", + "affPubRaw": "Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands" + } + ], + "name": { + "given_name": "R.", + "surname": "Aaij" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation50", + "affPubRaw": "Physik-Institut, Universit\u00e4t Z\u00fcrich, Z\u00fcrich, Switzerland" + } + ], + "name": { + "given_name": "C.", + "surname": "Abell\u00e1n\u00a0Beteta" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation60", + "affPubRaw": "Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom" + } + ], + "name": { + "given_name": "T.", + "surname": "Ackernley" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation46", + "affPubRaw": "Instituto Galego de F\u00edsica de Altas Enerx\u00edas (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain" + } + ], + "name": { + "given_name": "B.", + "surname": "Adeva" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation54", + "affPubRaw": "H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom" + } + ], + "name": { + "given_name": "M.", + "surname": "Adinolfi" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation09", + "affPubRaw": "Universit\u00e9 Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France" + } + ], + "name": { + "given_name": "H.", + "surname": "Afsharnia" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation85", + "affPubRaw": "University of Michigan, Ann Arbor, United States, associated to 68" + } + ], + "name": { + "given_name": "C.A.", + "surname": "Aidala" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation25", + "affPubRaw": "INFN Sezione di Milano, Milano, Italy" + } + ], + "name": { + "given_name": "S.", + "surname": "Aiola" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation09", + "affPubRaw": "Universit\u00e9 Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France" + } + ], + "name": { + "given_name": "Z.", + "surname": "Ajaltouni" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation65", + "affPubRaw": "University of Cincinnati, Cincinnati, OH, United States" + } + ], + "name": { + "given_name": "S.", + "surname": "Akar" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation15", + "affPubRaw": "Fakult\u00e4t Physik, Technische Universit\u00e4t Dortmund, Dortmund, Germany" + } + ], + "name": { + "given_name": "J.", + "surname": "Albrecht" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation48", + "affPubRaw": "European Organization for Nuclear Research (CERN), Geneva, Switzerland" + } + ], + "name": { + "given_name": "F.", + "surname": "Alessio" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation59", + "affPubRaw": "School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom" + } + ], + "name": { + "given_name": "M.", + "surname": "Alexander" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation45", + "affPubRaw": "ICCUB, Universitat de Barcelona, Barcelona, Spain" + } + ], + "name": { + "given_name": "A.", + "surname": "Alfonso\u00a0Albero" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation62", + "affPubRaw": "Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom" + } + ], + "name": { + "given_name": "Z.", + "surname": "Aliouche" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation38", + "affPubRaw": "Petersburg Nuclear Physics Institute NRC Kurchatov Institute (PNPI NRC KI), Gatchina, Russia" + } + ], + "name": { + "given_name": "G.", + "surname": "Alkhazov" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation55", + "affPubRaw": "Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom" + } + ], + "name": { + "given_name": "P.", + "surname": "Alvarez\u00a0Cartelle" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation02", + "affPubRaw": "Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil" + } + ], + "name": { + "given_name": "S.", + "surname": "Amato" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation11", + "affPubRaw": "Universit\u00e9 Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France" + } + ], + "name": { + "given_name": "Y.", + "surname": "Amhis" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation48", + "affPubRaw": "European Organization for Nuclear Research (CERN), Geneva, Switzerland" + } + ], + "name": { + "given_name": "L.", + "surname": "An" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation22", + "affPubRaw": "INFN Sezione di Firenze, Firenze, Italy" + } + ], + "name": { + "given_name": "L.", + "surname": "Anderlini" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation38", + "affPubRaw": "Petersburg Nuclear Physics Institute NRC Kurchatov Institute (PNPI NRC KI), Gatchina, Russia" + } + ], + "name": { + "given_name": "A.", + "surname": "Andreianov" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation21", + "affPubRaw": "INFN Sezione di Ferrara, Ferrara, Italy" + } + ], + "name": { + "given_name": "M.", + "surname": "Andreotti" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation17", + "affPubRaw": "Physikalisches Institut, Ruprecht-Karls-Universit\u00e4t Heidelberg, Heidelberg, Germany" + } + ], + "name": { + "given_name": "F.", + "surname": "Archilli" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation44", + "affPubRaw": "Institute for High Energy Physics NRC Kurchatov Institute (IHEP NRC KI), Protvino, Russia, Protvino, Russia" + } + ], + "name": { + "given_name": "A.", + "surname": "Artamonov" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation68", + "affPubRaw": "Syracuse University, Syracuse, NY, United States" + } + ], + "name": { + "given_name": "M.", + "surname": "Artuso" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation42", + "affPubRaw": "Yandex School of Data Analysis, Moscow, Russia" + } + ], + "name": { + "given_name": "K.", + "surname": "Arzymatov" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation10", + "affPubRaw": "Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France" + } + ], + "name": { + "given_name": "E.", + "surname": "Aslanides" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation50", + "affPubRaw": "Physik-Institut, Universit\u00e4t Z\u00fcrich, Z\u00fcrich, Switzerland" + } + ], + "name": { + "given_name": "M.", + "surname": "Atzeni" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation12", + "affPubRaw": "Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France" + } + ], + "name": { + "given_name": "B.", + "surname": "Audurier" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation17", + "affPubRaw": "Physikalisches Institut, Ruprecht-Karls-Universit\u00e4t Heidelberg, Heidelberg, Germany" + } + ], + "name": { + "given_name": "S.", + "surname": "Bachmann" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation49", + "affPubRaw": "Institute of Physics, Ecole Polytechnique F\u00e9d\u00e9rale de Lausanne (EPFL), Lausanne, Switzerland" + } + ], + "name": { + "given_name": "M.", + "surname": "Bachmayer" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation56", + "affPubRaw": "Department of Physics, University of Warwick, Coventry, United Kingdom" + } + ], + "name": { + "given_name": "J.J.", + "surname": "Back" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation46", + "affPubRaw": "Instituto Galego de F\u00edsica de Altas Enerx\u00edas (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain" + } + ], + "name": { + "given_name": "P.", + "surname": "Baladron\u00a0Rodriguez" + } + }, + { + "affiliation": [ + { + "affPubID": "affiliation12", + "affPubRaw": "Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France" + } + ], + "name": { + "given_name": "V.", + "surname": "Balagura" + } + }, + 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C20106834535410.1140/epjc/s10052-010-1350-2(arXiv:1004.3514)", + " LHCb Collaboration AaijRoel Measurement of charged particle multiplicities and densities in pp collisions at \u221a(s)=7TeV in the forward regionEur. Phys. J. C201474288810.1140/epjc/s10052-014-2888-1(arXiv:1402.4430)", + " ALICE Collaboration AbelevBetty Centrality determination of Pb-Pb collisions at \u221a(s_NN) = 2.76 TeV with ALICEPhys. Rev. C20138804490910.1103/PhysRevC.88.044909(arXiv:1301.4361)" + ], + "title": { + "textEnglish": "Centrality determination in heavy-ion collisions with the LHCb detector" + } +} diff --git a/tests/stubdata/output/jats_nature_natsd_12_7375.json b/tests/stubdata/output/jats_nature_natsd_12_7375.json new file mode 100644 index 0000000..9fb9f42 --- /dev/null +++ b/tests/stubdata/output/jats_nature_natsd_12_7375.json @@ -0,0 +1,1513 @@ +{ + "abstract": { + "textEnglish": "Gestational diabetes mellitus (GDM) plus rectus abdominis muscle (RAM) myopathy predicts long-term urinary incontinence (UI). Atrophic and stiff RAM are characteristics of diabetes-induced myopathy (DiM) in pregnant rats. This study aimed to determine whether swimming exercise (SE) has a therapeutic effect in mild hyperglycemic pregnant rats model. We hypothesized that SE training might help to reverse RAM DiM. Mild hyperglycemic pregnant rats model was obtained by a unique subcutaneous injection of 100 mg/kg streptozotocin (diabetic group) or citrate buffer (non-diabetic group) on the first day of life in Wistar female newborns. At 90 days of life, the rats are mated and randomly allocated to remain sedentary or subjected to a SE protocol. The SE protocol started at gestational day 0 and consisted of 60 min/day for 6 days/week in a period of 20 days in a swim tunnel. On day 21, rats were sacrificed, and RAM was collected and studied by picrosirius red, immunohistochemistry, and transmission electron microscopy. The SE protocol increased the fiber area and diameter, and the slow-twitch and fast-twitch fiber area and diameter in the diabetic exercised group, a finding was also seen in control sedentary animals. There was a decreased type I collagen but not type III collagen area and showed a similar type I/type III ratio compared with the control sedentary group. In conclusion, SE during pregnancy reversed the RAM DiM in pregnant rats. These findings may be a potential protocol to consider in patients with RAM damage caused by GDM." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "Aff1", + "affPubRaw": "Postgraduate Program on Tocogynecology, Department of Gynecology and Obstetrics, Botucatu Medical School S\u00e3o Paulo State University (UNESP) Botucatu S\u00e3o Paulo Brazil" + } + ], + "name": { + "given_name": "Bruna B.", + "surname": "Catinelli" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff2", + "affPubRaw": "Department of Physiotherapy and Occupational Therapy, School of Philosophy and Sciences S\u00e3o Paulo State University (UNESP) Mar\u00edlia S\u00e3o Paulo Brazil" + } + ], + "name": { + "given_name": "Patr\u00edcia S.", + "surname": "Rossignoli" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff1", + "affPubRaw": "Postgraduate Program on Tocogynecology, Department of Gynecology and Obstetrics, Botucatu Medical School S\u00e3o Paulo State University (UNESP) Botucatu S\u00e3o Paulo Brazil" + } + ], + "name": { + "given_name": "Juliana F.", + "surname": "Floriano" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff1", + "affPubRaw": "Postgraduate Program on Tocogynecology, Department of Gynecology and Obstetrics, Botucatu Medical School S\u00e3o Paulo State University (UNESP) Botucatu S\u00e3o Paulo Brazil" + } + ], + "name": { + "given_name": "Aline M.", + "surname": "Carr" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff1", + "affPubRaw": "Postgraduate Program on Tocogynecology, Department of Gynecology and Obstetrics, Botucatu Medical School S\u00e3o Paulo State University (UNESP) Botucatu S\u00e3o Paulo Brazil" + } + ], + "name": { + "given_name": "Rafael G.", + "surname": "de Oliveira" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff3", + "affPubRaw": "Laboratory of Extracellular Matrix Biology, Department of Structural and Functional Biology, Institute of Biosciences of Botucatu S\u00e3o Paulo State University (UNESP) Botucatu S\u00e3o Paulo Brazil" + }, + { + "affPubID": "Aff4", + "affPubRaw": "Department of Structural and Functional Biology, Institute of Biology (IB), UNICAMP University of Campinas (UNICAMP) Campinas S\u00e3o Paulo Brazil" + } + ], + "name": { + "given_name": "Nilton J.", + "surname": "dos Santos" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff5", + "affPubRaw": "University of Mar\u00edlia (UNIMAR) Mar\u00edlia S\u00e3o Paulo Brazil" + } + ], + "name": { + "given_name": "Lara C. 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Diabetes2011123453641:CAS:528:DC%2BC3MXoslOmu78%3D2086056110.1111/j.1399-5448.2010.00699.x", + "HansonMAGluckmanPDMaRCWMatzenPBiesmaRGEarly life opportunities for prevention of diabetes in low and middle income countriesBMC Public Health201212110.1186/1471-2458-12-1025", + "PoonLCMcIntyreHDHyettJAda FonsecaEBHodMThe first-trimester of pregnancy\u2014A window of opportunity for prediction and prevention of pregnancy complications and future lifeDiabetes Res. Clin. Pract.201814520302985223310.1016/j.diabres.2018.05.002", + "OrleansEDComparison betweent the effects of swimming and treadmill-based aerobic training protocols in diabetic ratsInt. J. Cardiovasc. 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Med.20169856671:CAS:528:DC%2BC28XltlOktbw%3D2703270910.1016/j.freeradbiomed.2016.03.025", + "MariniGde RinaldiJCDamascenoDCFelisbinoSLRudgeMVCAltera\u00e7\u00f5es da matriz extracelular causadas pelo diabetes: O impacto sobre a contin\u00eancia urin\u00e1riaRev. Bras. Ginecol. Obs.20143632833310.1590/SO100-720320140005014", + "MarangonLGobattoCde MelloMKEUtilization of an hyperbolic model for the determination of the critical load in swimming ratsMed. Sci. Sport. Exerc.20023414910.1097/00005768-200205001-00834", + "ManchadoFDBGobattoCAContartezeRVLPapotiMMMM\u00e1xima fase est\u00e1vel de lactato \u00e9 erg\u00f4metro-dependente em modelo experimental utilizando ratosRev. Bras. Med. Esporte2006625926210.1590/S1517-86922006000500007", + "VolpatoGTDamascenoDCKempinasWGRudgeMVCCalderonIMPEffect of exercise on the reproductive outcome and fetal development of diabetic ratsReprod. Biomed. Online2009198528581:STN:280:DC%2BD1Mfkt1Gitw%3D%3D2003102810.1016/j.rbmo.2009.09.027", + "DamascenoDCMild diabetes models and their maternal-fetal repercussionsJ. Diabetes Res.201320132610.1155/2013/473575", + "DamascenoDCStreptozotocin-induced diabetes models : Pathophysiological mechanisms and fetal outcomesBiomed. Res. Int.201412014", + "SinzatoYKDamascenoDCLaufer-AmorimRRodriguesMMPOshiiwaMTaylorKNPlasma concentrations and placental immunostaining of interleukin-10 and tumornecrosis factor-\u03b1 as predictors of alterations in the embryo-fetal organism and the placental development of diabetic ratsBraz. J. Med. Biol. Res.2011442062111:CAS:528:DC%2BC3MXlvVSlsrg%3D2134413910.1590/S0100-879X2011007500015", + "IessiILEvaluation of neonatally-induced mild diabetes in rats: Maternal and fetal repercussionsDiabetol. Metab. Syndr.201021810.1186/1758-5996-2-371:CAS:528:DC%2BC3cXnsVCjsb4%3D", + "Damasceno, D.C., Kempinas, W.G., Volpato, G.T., Consoni, M., Rudge, M.V.C., Paumgartten, F. Anomalias Cong\u00eanitas: Estudos Experimentais. (Coopmed, 2008).", + "Nascimento, L. Avalia\u00e7\u00e3o de diferentes modelos de indu\u00e7\u00e3o do diabete moderado em ratas Wistar e suas repercuss\u00f5es no organismo materno-fetal. (2014)." + ], + "title": { + "textEnglish": "Reversal of diabetic-induced myopathy by swimming exercise in pregnant rats: a translational intervention study" + } +} diff --git a/tests/stubdata/output/jats_pnas_119_2201344119.json b/tests/stubdata/output/jats_pnas_119_2201344119.json new file mode 100644 index 0000000..c489e23 --- /dev/null +++ b/tests/stubdata/output/jats_pnas_119_2201344119.json @@ -0,0 +1,71 @@ +{ + "authors": [ + { + "name": { + "given_name": "Beth", + "surname": "Azar" + } + } + ], + "copyright": { + "statement": "\u00a9 2022", + "status": true + }, + "openAccess": { + "license": "This article is distributed under Creative Commons Attribution-NonCommercial-NoDerivatives License 4.0 (CC BY-NC-ND).", + "licenseURL": "https://creativecommons.org/licenses/by-nc-nd/4.0/" + }, + "pagination": { + "electronicID": "e2201344119", + "pageCount": "2" + }, + "persistentIDs": [ + { + "DOI": "10.1073/pnas.2201344119" + } + ], + "pubDate": { + "electrDate": "2022-03-03", + "printDate": "2022-03-08" + }, + "publication": { + "ISSN": [ + { + "issnString": "0027-8424", + "pubtype": "ppub" + }, + { + "issnString": "1091-6490", + "pubtype": "epub" + } + ], + "issueNum": "10", + "pubName": "Proceedings of the National Academy of Sciences", + "pubYear": "2022", + "publisher": "National Academy of Sciences", + "volumeNum": "119" + }, + "publisherIDs": [ + { + "Identifier": "202201344", + "attribute": "publisher-id" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + "M. J. Moulton , Neuronal ROS-induced glial lipid droplet formation is altered by loss of Alzheimer\u2019s disease-associated genes. Proc. Natl. Acad. Sci. U.S.A. 118, e2112095118 (2021).", + "S. Yamamoto , A Drosophila genetic resource of mutants to study mechanisms underlying human genetic diseases. Cell 159, 200\u2013214 (2014).", + "L. Liu , Glial lipid droplets and ROS induced by mitochondrial defects promote neurodegeneration. Cell 160, 177\u2013190 (2015).", + "G. Lin , Phospholipase PLA2G6, a parkinsonism-associated gene, affects Vps26 and Vps35, retromer function, and ceramide levels, similar to \u03b1-synuclein gain. Cell Metab. 28, 605\u2013618.e6 (2018)." + ], + "title": { + "textEnglish": "QnAs with Hugo J. Bellen" + } +} diff --git a/tests/stubdata/output/jats_springer_cldy_84_1543.json b/tests/stubdata/output/jats_springer_cldy_84_1543.json new file mode 100644 index 0000000..e0fdd9b --- /dev/null +++ b/tests/stubdata/output/jats_springer_cldy_84_1543.json @@ -0,0 +1,363 @@ +{ + "abstract": { + "textEnglish": "For decades, scaled analog experiments have improved the understanding of a broad range of multiphase volcanological processes in controlled laboratory environments. Successfully modeled processes include magma flow through magma reservoirs, conduits and sheets, associated crustal deformation, lava flow, volcanic plume dynamics, ash cloud dispersion, pyroclast sedimentation, pyroclastic density currents, and debris flows. Prior to the advent of computational modeling in volcanology, analog experiments were the primary method used to test newly developed concepts. Over the past two decades, technological advances have led to increased quantification of model observables, including deformation fields, lava flow rheologies, bubble and particle suspension compositions, runout distances, plume geometries, and rates of ash cloud spreading and sedimentation. For experimental results to yield further insights into volcanic processes and observables directly useful to volcano monitoring efforts, we expect future progress to focus on three major fronts: (1) improved multimethod measurements in experiments; (2) upscaling to near-natural-scale experiments conducted by multidisciplinary teams at internationally shared facilities; and (3) integration with computational models that will guide future geophysical observations and predictions of volcanic activity. This way, analog experiments will bridge gaps between other techniques in volcanology and improve our understanding and forecasting of volcanic activity from the Earth\u2019s mantle to the surface and into the atmosphere." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "Aff1", + "affPubRaw": "Centrum Bada\u0144 Kosmicznych Polskiej Akademii Nauk (CBK PAN) Bartycka 18A 00-716 Warszawa, Warsaw Poland" + }, + { + "affPubID": "Aff2", + "affPubRaw": "Laboratoire G-Time, Department of Geosciences, Environment and Society Universit\u00e9 Libre de Bruxelles Brussels Belgium" + } + ], + "attrib": { + "email": "sampoppe@cbk.waw.pl", + "orcid": "0000-0002-8787-8590" + }, + "name": { + "given_name": "Sam", + "surname": "Poppe" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff3", + "affPubRaw": "Geological Fluid Dynamics Laboratory, Department of Earth, Ocean and Atmospheric Sciences University of British Columbia Vancouver Canada" + }, + { + "affPubID": "Aff4", + "affPubRaw": "Department of Earth Sciences University of Oregon Eugene OR USA" + } + ], + "name": { + "given_name": "Johan T.", + "surname": "Gilchrist" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff4", + "affPubRaw": "Department of Earth Sciences University of Oregon Eugene OR USA" + }, + { + "affPubID": "Aff5", + "affPubRaw": "School of Geosciences University of Edinburgh, The King\u2019s Building Edinburgh UK" + } + ], + "attrib": { + "orcid": "0000-0001-8756-8202" + }, + "name": { + "given_name": "Eric Christophe Pascal", + "surname": "Breard" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff6", + "affPubRaw": "Department of Earth and Environmental Sciences University of Missouri Kansas City Kansas City MO USA" + } + ], + "attrib": { + "orcid": "0000-0003-2831-9446" + }, + "name": { + "given_name": "Alison", + "surname": "Graettinger" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff7", + "affPubRaw": "Department of Earth Science Durham University Durham UK" + } + ], + "attrib": { + "orcid": "0000-0001-6267-0411" + }, + "name": { + "given_name": "Stephen", + "surname": "Pansino" + } + } + ], + "copyright": { + "statement": "\u00a9 International Association of Volcanology & Chemistry of the Earth's Interior 2022", + "status": true + }, + "editorialHistory": { + "acceptedDate": "2022-02-10", + "receivedDates": [ + "2021-10-15" + ] + }, + "funding": [ + { + "agencyid": { + "idschema": "doi", + "idvalue": "http://dx.doi.org/10.13039/501100004281" + }, + "agencyname": "Narodowe Centrum Nauki", + "awardnumber": "2020/37/K/ST10/02447" + }, + { + "agencyid": { + "idschema": "doi", + "idvalue": "http://dx.doi.org/10.13039/501100002661" + }, + "agencyname": "Fonds De La Recherche Scientifique - FNRS" + }, + { + "agencyid": { + "idschema": "doi", + "idvalue": "http://dx.doi.org/10.13039/501100002790" + }, + "agencyname": "Canadian Network for Research and Innovation in Machining Technology, Natural Sciences and Engineering Research Council of Canada" + }, + { + "agencyid": { + "idschema": "doi", + "idvalue": "http://dx.doi.org/10.13039/100000001" + }, + "agencyname": "National Science Foundation", + "awardnumber": "1852569" + }, + { + "agencyname": "Royal Society - Newton International Fellowship", + "awardnumber": "NIF\\R1\\202137" + } + ], + "keywords": [ + { + "keyString": "Analog modeling", + "keySystem": "misc" + }, + { + "keyString": "Laboratory experiments", + "keySystem": "misc" + }, + { + "keyString": "Magma intrusion", + "keySystem": "misc" + }, + { + "keyString": "Pyroclastic density currents", + "keySystem": "misc" + }, + { + "keyString": "Explosive eruptions", + "keySystem": "misc" + } + ], + "pagination": { + "electronicID": "52" + }, + "persistentIDs": [ + { + "DOI": "10.1007/s00445-022-01543-x" + } + ], + "pubDate": { + "electrDate": "2022-05-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "1432-0819", + "pubtype": "epub" + } + ], + "issueNum": "5", + "pubName": "Bulletin of Volcanology", + "pubYear": "2022", + "publisher": "Springer Berlin Heidelberg", + "volumeNum": "84" + }, + "publisherIDs": [ + { + "Identifier": "s00445-022-01543-x", + "attribute": "publisher-id" + }, + { + "Identifier": "1543", + "attribute": "manuscript" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + " Abdelmalak MM Bulois C Mourgues R Description of new dry granular materials of variable cohesion and friction coefficient: implications for laboratory modeling of the brittle crust Tectonophysics 2016 684 39 51 10.1016/j.tecto.2016.03.003 ", + " Acocella V Understanding caldera structure and development: an overview of analogue models compared to natural calderas Earth-Science Rev 2007 85 125 160 10.1016/j.earscirev.2007.08.004 ", + " Albino F Biggs J Yu C Li Z Automated methods for detecting volcanic deformation using Sentinel-1 InSAR time series illustrated by the 2017\u20132018 unrest at Agung, Indonesia J Geophys Res Solid Earth 2020 125 1 40 10.1029/2019JB017908 ", + " Alfano F, Bonadonna C, Watt S et al (2016) Reconstruction of total grain size distribution of the climactic phase of a long-lasting eruption: the example of the 2008\u20132013 Chait\u00e9n eruption. 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Data were collected with the CMS detector at the LHC in 2016\u20132018, corresponding to an integrated luminosity of 138 fb \u22121 . Resonances with a mass between 0.8 and 4.5 TeV are considered using events in which one Higgs boson decays into a bottom quark pair and the other into final states with either one or two charged leptons. Specifically, the single-lepton decay channel HH \u2192 b b \u00af WW \u2217 \u2192 b b \u00af \u2113 v q q \u00af \u2032 \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ \\mathrm{HH}\\to \\mathrm{b}\\overline{\\mathrm{b}}{\\mathrm{WW}}^{\\ast}\\to \\mathrm{b}\\overline{\\mathrm{b}}\\ell v\\mathrm{q}{\\overline{\\mathrm{q}}}^{\\prime } $$\\end{document} and the dilepton decay channels HH \u2192 b b \u00af WW \u2217 \u2192 b b \u00af \u2113 v \u2113 v \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ \\mathrm{HH}\\to \\mathrm{b}\\overline{\\mathrm{b}}{\\mathrm{WW}}^{\\ast}\\to \\mathrm{b}\\overline{\\mathrm{b}}\\ell v\\ell v $$\\end{document} and HH \u2192 b b \u00af \u03c4\u03c4 \u2192 b b \u00af \u2113 vv \u2113 vv \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ \\mathrm{HH}\\to \\mathrm{b}\\overline{\\mathrm{b}}\\uptau \\uptau \\to \\mathrm{b}\\overline{\\mathrm{b}}\\ell vv\\ell vv $$\\end{document} are examined, where \u2113 in the final state corresponds to an electron or muon. The signal is extracted using a two-dimensional maximum likelihood fit of the H \u2192 b b \u00af \\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ \\mathrm{H}\\to \\mathrm{b}\\overline{\\mathrm{b}} $$\\end{document} jet mass and HH invariant mass distributions. No significant excess above the standard model expectation is observed in data. Model-independent exclusion limits are placed on the product of the cross section and branching fraction for narrow spin-0 and spin-2 massive bosons decaying to HH. The results are also interpreted in the context of radion and bulk graviton production in models with a warped extra spatial dimension. The results provide the most stringent limits to date for X \u2192 HH signatures with final-state leptons and at some masses provide the most sensitive limits of all X \u2192 HH searches.\n[graphic not available: see fulltext]" + }, + "authors": [ + { + "attrib": { + "collab": true + }, + "name": { + "collab": "The CMS collaboration" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff1", + "affPubRaw": "Yerevan Physics Institute Yerevan Armenia" + } + ], + "name": { + "given_name": "A.", + "surname": "Tumasyan" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff2", + "affPubRaw": "Institut f\u00fcr Hochenergiephysik Vienna Austria" + } + ], + "attrib": { + "orcid": "0000-0001-9099-4341" + }, + "name": { + "given_name": "W.", + "surname": "Adam" + } + }, + { + "affiliation": [ + { + "affPubID": "Aff2", + "affPubRaw": "Institut f\u00fcr Hochenergiephysik Vienna Austria" + } + ], + "name": { + "given_name": "J. 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This article is distributed under the terms of the Creative Commons Attribution License (\n\t\t\t\t\t\tCC-BY 4.0), which permits any use, distribution and reproduction in any medium, provided the original author(s) and source are credited.\n\t\t\t\t\t", + "licenseURL": "http://creativecommons.org/licenses/by/4.0/", + "open": true + }, + "pagination": { + "electronicID": "5" + }, + "persistentIDs": [ + { + "DOI": "10.1007/JHEP05(2022)005" + } + ], + "pubDate": { + "electrDate": "2022-05-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "1029-8479", + "pubtype": "epub" + } + ], + "issueNum": "5", + "pubName": "Journal of High Energy Physics", + "pubYear": "2022", + "publisher": "Springer Berlin Heidelberg", + "volumeNum": "2022" + }, + "publisherIDs": [ + { + "Identifier": "JHEP05(2022)005", + "attribute": "publisher-id" + }, + { + "Identifier": "18294", + "attribute": "manuscript" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + " ATLAS collaboration, \t\t\t\t\t\tObservation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC, \t\t\t\t\t\tPhys. 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Phys. J. C 78 (2018) 293 [ \t\t\t\t\t\tarXiv:1712.06386] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " ATLAS collaboration, \t\t\t\t\t\tSearch for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 \t\t\t\t\t\tfb \u22121 \t\t\t\t\t\t of \t\t\t\t\t\t s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 \t\t\t\t\t\tTeV pp collisions with the ATLAS detector, \t\t\t\t\t\tJHEP 03 (2018) 174 [ \t\t\t\t\t\tErratum ibid. 11 (2018) 051] [ \t\t\t\t\t\tarXiv:1712.06518] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " ATLAS collaboration, \t\t\t\t\t\tSearch for Higgs boson pair production in the b b \u00af \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\overline{b} $$\\end{document} WW * decay mode at s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 \t\t\t\t\t\tTeV with the ATLAS detector, \t\t\t\t\t\tJHEP 04 (2019) 092 [ \t\t\t\t\t\tarXiv:1811.04671] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " ATLAS collaboration, \t\t\t\t\t\tSearch for diboson resonances in hadronic final states in 139 \t\t\t\t\t\tfb \u22121 \t\t\t\t\t\t of pp collisions at s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 \t\t\t\t\t\tTeV with the ATLAS detector, \t\t\t\t\t\tJHEP 09 (2019) 091 [ \t\t\t\t\t\tErratum ibid. 06 (2020) 042] [ \t\t\t\t\t\tarXiv:1906.08589] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " ATLAS collaboration, \t\t\t\t\t\tSearch for the HH \u2192 \t\t\t\t\t\tb b \u00af \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\overline{b} $$\\end{document} b b \u00af \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\overline{b} $$\\end{document} process via vector-boson fusion production using proton-proton collisions at s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 \t\t\t\t\t\tTeV with the ATLAS detector, \t\t\t\t\t\tJHEP 07 (2020) 108 [ \t\t\t\t\t\tErratum ibid. 01 (2021) 145] [ \t\t\t\t\t\tErratum ibid. 05 (2021) 207] [ \t\t\t\t\t\tarXiv:2001.05178] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " ATLAS collaboration, \t\t\t\t\t\tSearch for heavy diboson resonances in semileptonic final states in pp collisions at s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 \t\t\t\t\t\tTeV with the ATLAS detector, \t\t\t\t\t\tEur. Phys. J. C 80 (2020) 1165 [ \t\t\t\t\t\tarXiv:2004.14636] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " ATLAS collaboration, \t\t\t\t\t\tSearch for resonances decaying into a weak vector boson and a Higgs boson in the fully hadronic final state produced in proton\u2212proton collisions at s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 \t\t\t\t\t\tTeV with the ATLAS detector, \t\t\t\t\t\tPhys. Rev. D 102 (2020) 112008 [ \t\t\t\t\t\tarXiv:2007.05293] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " ATLAS collaboration, \t\t\t\t\t\tReconstruction and identification of boosted di-\u03c4 systems in a search for Higgs boson pairs using 13 \t\t\t\t\t\tTeV proton-proton collision data in ATLAS, \t\t\t\t\t\tJHEP 11 (2020) 163 [ \t\t\t\t\t\tarXiv:2007.14811] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " ATLAS collaboration, \t\t\t\t\t\tSearch for resonant pair production of Higgs bosons in the b b \u00af \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\overline{b} $$\\end{document} b b \u00af \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\overline{b} $$\\end{document} final state using pp collisions at s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 \t\t\t\t\t\tTeV with the ATLAS detector, \t\t\t\t\t\tarXiv:2202.07288 [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " ATLAS collaboration, \t\t\t\t\t\tCombination of searches for heavy resonances decaying into bosonic and leptonic final states using 36 \t\t\t\t\t\tfb \u22121 \t\t\t\t\t\t of proton-proton collision data at s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 \t\t\t\t\t\tTeV with the ATLAS detector, \t\t\t\t\t\tPhys. Rev. D 98 (2018) 052008 [ \t\t\t\t\t\tarXiv:1808.02380] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " CMS collaboration, \t\t\t\t\t\tCombination of searches for heavy resonances decaying to WW, WZ, ZZ, WH, and ZH boson pairs in proton-proton collisions at s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 8 \t\t\t\t\t\tand 13 \t\t\t\t\t\tTeV, \t\t\t\t\t\tPhys. Lett. B 774 (2017) 533 [ \t\t\t\t\t\tarXiv:1705.09171] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " CMS collaboration, \t\t\t\t\t\tSearch for heavy resonances decaying into two Higgs bosons or into a Higgs boson and a W or Z boson in proton-proton collisions at 13 \t\t\t\t\t\tTeV, \t\t\t\t\t\tJHEP 01 (2019) 051 [ \t\t\t\t\t\tarXiv:1808.01365] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " CMS collaboration, \t\t\t\t\t\tSearch for a heavy resonance decaying into a Z boson and a Z or W boson in 2 \t\t\t\t\t\t\u21132 \t\t\t\t\t\tq final states at s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 \t\t\t\t\t\tTeV, \t\t\t\t\t\tJHEP 09 (2018) 101 [ \t\t\t\t\t\tarXiv:1803.10093] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " CMS collaboration, \t\t\t\t\t\tSearch for production of Higgs boson pairs in the four b quark final state using large-area jets in proton-proton collisions at s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 \t\t\t\t\t\tTeV, \t\t\t\t\t\tJHEP 01 (2019) 040 [ \t\t\t\t\t\tarXiv:1808.01473] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " CMS collaboration, \t\t\t\t\t\tSearch for massive resonances decaying into WW, WZ, ZZ, qW, and qZ with dijet final states at s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 \t\t\t\t\t\tTeV, \t\t\t\t\t\tPhys. 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Lett. 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\\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 \t\t\t\t\t\tTeV, \t\t\t\t\t\tarXiv:2109.08268 [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " CMS collaboration, \t\t\t\t\t\tSearch for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production at s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 \t\t\t\t\t\tTeV, \t\t\t\t\t\tarXiv:2111.13669 [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " CMS collaboration, \t\t\t\t\t\tSearch for resonances decaying to a pair of Higgs bosons in the b b \u00af \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\overline{b} $$\\end{document} q q \u00af \u2032 \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ {\\overline{q}}^{\\prime } $$\\end{document} \u2113 \t\t\t\t\t\t\u03bd final state in proton-proton collisions at s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} 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collaboration, \t\t\t\t\t\tThe CMS experiment at the CERN LHC, 2008 \t\t\t\t\t\tJINST 3 S08004 [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " CMS collaboration, \t\t\t\t\t\tPerformance of the CMS Level-1 trigger in proton-proton collisions at s \\documentclass[12pt]{minimal} \t\t\t\t\\usepackage{amsmath} \t\t\t\t\\usepackage{wasysym} \t\t\t\t\\usepackage{amsfonts} \t\t\t\t\\usepackage{amssymb} \t\t\t\t\\usepackage{amsbsy} \t\t\t\t\\usepackage{mathrsfs} \t\t\t\t\\usepackage{upgreek} \t\t\t\t\\setlength{\\oddsidemargin}{-69pt} \t\t\t\t\\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 \t\t\t\t\t\tTeV, 2020 \t\t\t\t\t\tJINST 15 P10017 [ \t\t\t\t\t\tarXiv:2006.10165] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " CMS collaboration, \t\t\t\t\t\tThe CMS trigger system, 2017 \t\t\t\t\t\tJINST 12 P01020 [ \t\t\t\t\t\tarXiv:1609.02366] [ \t\t\t\t\t\tINSPIRE]. \t\t\t\t\t ", + " CMS collaboration, \t\t\t\t\t\tParticle-flow reconstruction and global event description with the CMS detector, 2017 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Southern Africa (SA) is susceptible and vulnerable to drought due to its type of climate. In the last four decades, droughts have occurred more frequently, with increasing intensity and impacts on ecosystems, agriculture, and health. The work consists of a systematic literature review on the drought regime\u2019s characteristics in the SA under current and future climatic conditions, conducted on the Web of Science and Scopus platforms, using the PRISMA2020 methodology, with usual and appropriate inclusion and exclusion criteria to minimize/eliminate the risk of bias, which lead to 53 documents published after the year 1987. The number of publications on the drought regime in SA is still very small. The country with the most drought situations studied is South Africa, and the countries with fewer studies are Angola and Namibia. The analysis revealed that the main driver of drought in SA is the ocean\u2013atmosphere interactions, including the El Ni\u00f1o Southern Oscillation. The documents used drought indices, evaluating drought descriptors for some regions, but it was not possible to identify one publication that reports the complete study of the drought regime, including the spatial and temporal distribution of all drought descriptors in SA." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "af1-climate-11-00147", + "affPubRaw": "Centre for Research and Technology of Agro-Environmental and Biological Sciences (CITAB), Inov4Agro, University of Tr\u00e1s-os-Montes and Alto Douro (UTAD), Quinta de Prados, 5000-801 Vila Real, Portugal" + } + ], + "attrib": { + "orcid": "0000-0003-0332-1910" + }, + "name": { + "given_name": "Fernando Maliti", + "surname": "Chivangulula" + } + }, + { + "affiliation": [ + { + "affPubID": "af1-climate-11-00147", + "affPubRaw": "Centre for Research and Technology of Agro-Environmental and Biological Sciences (CITAB), Inov4Agro, University of Tr\u00e1s-os-Montes and Alto Douro (UTAD), Quinta de Prados, 5000-801 Vila Real, Portugal" + } + ], + "name": { + "given_name": "Malik", + "surname": "Amraoui" + } + }, + { + "affiliation": [ + { + "affPubID": "af1-climate-11-00147", + "affPubRaw": "Centre for Research and Technology of Agro-Environmental and Biological Sciences (CITAB), Inov4Agro, University of Tr\u00e1s-os-Montes and Alto Douro (UTAD), Quinta de Prados, 5000-801 Vila Real, Portugal" + }, + { + "affPubID": "af2-climate-11-00147", + "affPubRaw": "Instituto Dom Luiz (IDL), FCUL, Campo Grande Edif\u00edcio C1, Piso 1, 1749-016 Lisboa, Portugal" + } + ], + "attrib": { + "email": "gpereira@utad.pt", + "orcid": "0000-0001-6603-7453" + }, + "name": { + "given_name": "M\u00e1rio Gonzalez", + "surname": "Pereira" + } + } + ], + "copyright": { + "statement": "\u00a9 2023 by the authors.", + "status": true + }, + "editorialHistory": { + "acceptedDate": "2023-07-11", + "receivedDates": [ + "2023-06-09" + ], + "revisedDates": [ + "2023-07-02" + ] + }, + "funding": [ + { + "agencyname": "FCT\u2014Portuguese Foundation for Science and Technology", + "awardnumber": "UIDB/04033/2020" + } + ], + "keywords": [ + { + "keyString": "drought regime", + "keySystem": "misc" + }, + { + "keyString": "Southern Africa", + "keySystem": "misc" + }, + { + "keyString": "drought factors", + "keySystem": "misc" + }, + { + "keyString": "drought impacts", + "keySystem": "misc" + }, + { + "keyString": "drought indices", + "keySystem": "misc" + } + ], + "openAccess": { + "license": "Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).", + "licenseURL": "https://creativecommons.org/licenses/by/4.0/", + "open": true + }, + "otherContributor": [ + { + "contrib": { + "name": { + "given_name": "Rui A. P.", + "surname": "Perdig\u00e3o" + } + }, + "role": "Academic Editor" + } + ], + "pagination": { + "electronicID": "147" + }, + "persistentIDs": [ + { + "DOI": "10.3390/cli11070147" + } + ], + "pubDate": { + "electrDate": "2023-07-13" + }, + "publication": { + "ISSN": [ + { + "issnString": "2225-1154", + "pubtype": "epub" + } + ], + "issueNum": "7", + "pubName": "Climate", + "pubYear": "2023", + "publisher": "MDPI", + "volumeNum": "11" + }, + "publisherIDs": [ + { + "Identifier": "climate-11-00147", + "attribute": "publisher-id" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + " IPCC Summary for Policymakers Global Warming of 1.5 \u00b0C. 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Ngwenya N. Seeley J. Hanekom W. Herbst K. Kniveton D. Exploring Linkages between Drought and HIV Treatment Adherence in Africa: A Systematic Review Lancet Planet. Health 2022 6 e359 e370 10.1016/S2542-5196(22)00016-X ", + " O\u2019farrell P.J. Anderson P.M.L. Milton S.J. Dean W.R.J. Human Response and Adaptation to Drought in the Arid Zone: Lessons from Southern Africa S. Afr. J. Sci. 2009 105 34 39 10.10520/EJC96878 ", + " Samways M.J. Deacon C. Kietzka G.J. Pryke J.S. Vorster C. Simaika J.P. Value of Artificial Ponds for Aquatic Insects in Drought-Prone Southern Africa: A Review Biodivers. Conserv. 2020 29 3131 3150 10.1007/s10531-020-02020-7 ", + " Dean W.R.J. Barnard P. Anderson M.D. When to Stay, When to Go: Trade-Offs for Southern African Arid-Zone Birds in Times of Drought S. Afr. J. Sci. 2009 105 24 28 10.4102/sajs.v105i1/2.7 " + ], + "title": { + "textEnglish": "The Drought Regime in Southern Africa: A Systematic Review" + } +} diff --git a/tests/stubdata/output/mdpi_galaxies-11-00090.json b/tests/stubdata/output/mdpi_galaxies-11-00090.json new file mode 100644 index 0000000..5d90afd --- /dev/null +++ b/tests/stubdata/output/mdpi_galaxies-11-00090.json @@ -0,0 +1,240 @@ +{ + "abstract": { + "textEnglish": "The IR spectra of Be stars display numerous hydrogen recombination lines, constituting a great resource for obtaining information on the physical and dynamic structures of different regions within the circumstellar envelope. Nevertheless, this spectral region has not been analysed in depth, and there is a lack of synthetic spectra with which to compare observations. Therefore, we computed synthetic spectra with the HDUST code for different disc parameters. Here, we present our results on the spectral region that includes lines of the Brackett series. We discuss the dependence of the line series strengths on several parameters that describe the structure of the disc. We also compared model line profiles, fluxes, and EWs with observational data for two Be stars (MX Pup and \u03c0 Aqr). Even though the synthetic spectra adequately fit our observations of both stars and allow us to constrain the parameters of the disc, there is a discrepancy with the observed data in the EW and flux measurements, especially in the case of MX Pup. It is possible that by including Brackett lines of higher terms or adding the analysis of other series, we may be able to better constrain the parameters of the observed disc." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "af1-galaxies-11-00090", + "affPubRaw": "Instituto de Astrof\u00edsica de La Plata (CCT La Plata\u2014CONICET, UNLP), Paseo del Bosque S/N, La Plata B1900FWA, Argentina" + }, + { + "affPubID": "af2-galaxies-11-00090", + "affPubRaw": "Departamento de Espectroscop\u00eda, Facultad de Ciencias Astron\u00f3micas y Geof\u00edsicas, Universidad Nacional de La Plata, La Plata B1900FWA, Argentina" + } + ], + "attrib": { + "email": "cochetti@fcaglp.unlp.edu.ar", + "orcid": "0000-0002-2763-7250" + }, + "name": { + "given_name": "Yanina Roxana", + "surname": "Cochetti" + } + }, + { + "affiliation": [ + { + "affPubID": "af3-galaxies-11-00090", + "affPubRaw": "Centro Interdisciplinario de Telecomunicaciones, Electr\u00f3nica, Computaci\u00f3n y Ciencia Aplicada (CITECCA), Sede Andina, Universidad Nacional de R\u00edo Negro, San Carlos de Bariloche R8400AHN, Argentina" + } + ], + "name": { + "given_name": "Anahi", + "surname": "Granada" + } + }, + { + "affiliation": [ + { + "affPubID": "af1-galaxies-11-00090", + "affPubRaw": "Instituto de Astrof\u00edsica de La Plata (CCT La Plata\u2014CONICET, UNLP), Paseo del Bosque S/N, La Plata B1900FWA, Argentina" + }, + { + "affPubID": "af2-galaxies-11-00090", + "affPubRaw": "Departamento de Espectroscop\u00eda, Facultad de Ciencias Astron\u00f3micas y Geof\u00edsicas, Universidad Nacional de La Plata, La Plata B1900FWA, Argentina" + } + ], + "attrib": { + "orcid": "0000-0002-4016-2501" + }, + "name": { + "given_name": "Mar\u00eda Laura", + "surname": "Arias" + } + }, + { + "affiliation": [ + { + "affPubID": "af1-galaxies-11-00090", + "affPubRaw": "Instituto de Astrof\u00edsica de La Plata (CCT La Plata\u2014CONICET, UNLP), Paseo del Bosque S/N, La Plata B1900FWA, Argentina" + }, + { + "affPubID": "af2-galaxies-11-00090", + "affPubRaw": "Departamento de Espectroscop\u00eda, Facultad de Ciencias Astron\u00f3micas y Geof\u00edsicas, Universidad Nacional de La Plata, La Plata B1900FWA, Argentina" + } + ], + "name": { + "given_name": "Andrea Fabiana", + "surname": "Torres" + } + }, + { + "affiliation": [ + { + "affPubID": "af4-galaxies-11-00090", + "affPubRaw": "Instituto de F\u00edsica y Astronom\u00eda, Facultad de Ciencias, Universidad de Valpara\u00edso, Valpara\u00edso 2360102, Chile" + } + ], + "attrib": { + "orcid": "0000-0002-4825-4910" + }, + "name": { + "given_name": "Catalina", + "surname": "Arcos" + } + } + ], + "copyright": { + "statement": "\u00a9 2023 by the authors.", + "status": true + }, + "editorialHistory": { + "acceptedDate": "2023-08-11", + "receivedDates": [ + "2023-03-14" + ], + "revisedDates": [ + "2023-08-09" + ] + }, + "funding": [ + { + "agencyname": "CONICET fellowship" + }, + { + "agencyname": "Universidad Nacional de La Plata", + "awardnumber": "11/G160" + }, + { + "agencyname": "CONICET", + "awardnumber": "28720210100879CO" + }, + { + "agencyname": "Fondecyt Regular", + "awardnumber": "1230131" + }, + { + "agencyname": "European Union\u2019s Framework Programme for Research and Innovation Horizon 2020 (2014\u20132020)", + "awardnumber": "823734" + } + ], + "keywords": [ + { + "keyString": "stars: early-type", + "keySystem": "misc" + }, + { + "keyString": "stars: emission-line, Be", + "keySystem": "misc" + }, + { + "keyString": "stars: individual: MX Pup, \u03c0 Aqr", + "keySystem": "misc" + }, + { + "keyString": "circumstellar matter", + "keySystem": "misc" + } + ], + "openAccess": { + "license": "Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).", + "licenseURL": "https://creativecommons.org/licenses/by/4.0/", + "open": true + }, + "otherContributor": [ + { + "contrib": { + "name": { + "given_name": "Jorick Sandor", + "surname": "Vink" + } + }, + "role": "Academic Editor" + } + ], + "pagination": { + "electronicID": "90" + }, + "persistentIDs": [ + { + "DOI": "10.3390/galaxies11040090" + } + ], + "pubDate": { + "electrDate": "2023-08-17" + }, + "publication": { + "ISSN": [ + { + "issnString": "2075-4434", + "pubtype": "epub" + } + ], + "issueNum": "4", + "pubName": "Galaxies", + "pubYear": "2023", + "publisher": "MDPI", + "volumeNum": "11" + }, + "publisherIDs": [ + { + "Identifier": "galaxies-11-00090", + "attribute": "publisher-id" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + " Jaschek M. 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J. 2022 935 167 10.3847/1538-4357/ac7c74 " + ], + "title": { + "textEnglish": "Infrared Spectroscopy of Be Stars: Influence of the Envelope Parameters on Brackett-Series Behaviour" + } +} diff --git a/tests/stubdata/output/mdpi_symmetry-15-00939.json b/tests/stubdata/output/mdpi_symmetry-15-00939.json new file mode 100644 index 0000000..3eda20a --- /dev/null +++ b/tests/stubdata/output/mdpi_symmetry-15-00939.json @@ -0,0 +1,231 @@ +{ + "abstract": { + "textEnglish": "One of the most important problems in the study of geometric function theory is knowing how to obtain the sharp bounds of the coefficients that appear in the Taylor\u2013Maclaurin series of univalent functions. In the present investigation, our aim is to calculate some sharp estimates of problems involving coefficients for the family of convex functions with respect to symmetric points and associated with a hyperbolic tangent function. These problems include the first four initial coefficients, the Fekete\u2013Szeg\u00f6 and Zalcman inequalities, and the second-order Hankel determinant. Additionally, the inverse and logarithmic coefficients of the functions belonging to the defined class are also studied in relation to the current problems." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "af1-symmetry-15-00939", + "affPubRaw": "Department of Mathematics, Abdul Wali Khan University Mardan, Mardan 23200, Pakistan" + } + ], + "name": { + "given_name": "Khalil", + "surname": "Ullah" + } + }, + { + "affiliation": [ + { + "affPubID": "af2-symmetry-15-00939", + "affPubRaw": "Department of Mathematics, The University of Jordon, Amman 11942, Jordan" + } + ], + "attrib": { + "email": "i.shbeil@ju.edu.jo", + "orcid": "0000-0001-5287-4656" + }, + "name": { + "given_name": "Isra", + "surname": "Al-Shbeil" + } + }, + { + "affiliation": [ + { + "affPubID": "af3-symmetry-15-00939", + "affPubRaw": "Department of Mathematics, Taibah University, Universities Road, P.O. Box 344, Medina 42353, Saudi Arabia" + } + ], + "attrib": { + "orcid": "0000-0002-4169-4366" + }, + "name": { + "given_name": "Muhammad Imran", + "surname": "Faisal" + } + }, + { + "affiliation": [ + { + "affPubID": "af1-symmetry-15-00939", + "affPubRaw": "Department of Mathematics, Abdul Wali Khan University Mardan, Mardan 23200, Pakistan" + } + ], + "attrib": { + "orcid": "0000-0003-1484-7643" + }, + "name": { + "given_name": "Muhammad", + "surname": "Arif" + } + }, + { + "affiliation": [ + { + "affPubID": "af4-symmetry-15-00939", + "affPubRaw": "Department of Mathematics, College of Science, King Saud University, P.O. Box 22452, Riyadh 11495, Saudi Arabia" + } + ], + "name": { + "given_name": "Huda", + "surname": "Alsaud" + } + } + ], + "copyright": { + "statement": "\u00a9 2023 by the authors.", + "status": true + }, + "editorialHistory": { + "acceptedDate": "2023-04-14", + "receivedDates": [ + "2023-03-23" + ], + "revisedDates": [ + "2023-04-11" + ] + }, + "keywords": [ + { + "keyString": "convex functions with respect to symmetric points", + "keySystem": "misc" + }, + { + "keyString": "subordinations", + "keySystem": "misc" + }, + { + "keyString": "Zalcman functionals", + "keySystem": "misc" + }, + { + "keyString": "logarithmic and inverse coefficients", + "keySystem": "misc" + }, + { + "keyString": "Hankel determinant problems", + "keySystem": "misc" + } + ], + "openAccess": { + "license": "Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).", + "licenseURL": "https://creativecommons.org/licenses/by/4.0/", + "open": true + }, + "otherContributor": [ + { + "contrib": { + "name": { + "given_name": "\u015eahsene", + "surname": "Alt\u0131nkaya" + } + }, + "role": "Academic Editor" + } + ], + "pagination": { + "electronicID": "939" + }, + "persistentIDs": [ + { + "DOI": "10.3390/sym15040939" + } + ], + "pubDate": { + "electrDate": "2023-04-19" + }, + "publication": { + "ISSN": [ + { + "issnString": "2073-8994", + "pubtype": "epub" + } + ], + "issueNum": "4", + "pubName": "Symmetry", + "pubYear": "2023", + "publisher": "MDPI", + "volumeNum": "15" + }, + "publisherIDs": [ + { + "Identifier": "symmetry-15-00939", + "attribute": "publisher-id" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + " Bieberbach L. \u00dcber di\u00e9 koeffizienten derjenigen Potenzreihen, welche eine schlichte Abbildung des Einheitskreises vermitteln Sitzungsberichte Preuss. 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Results on Hankel determinants for the inverse of certain analytic functions subordinated to the exponential function Mathematics 2022 10 3429 10.3390/math10193429 " + ], + "title": { + "textEnglish": "Results on Second-Order Hankel Determinants for Convex Functions with Symmetric Points" + } +} diff --git a/tests/stubdata/output/mdpi_universe-08-00651.json b/tests/stubdata/output/mdpi_universe-08-00651.json new file mode 100644 index 0000000..291a918 --- /dev/null +++ b/tests/stubdata/output/mdpi_universe-08-00651.json @@ -0,0 +1,270 @@ +{ + "abstract": { + "textEnglish": "We investigate the dependence of elemental abundances on physical constants, and the implications this has for the distribution of complex life for various proposed habitability criteria. We consider three main sources of abundance variation: differing supernova rates, alpha burning in massive stars, and isotopic stability, and how each affects the metal-to-rock ratio and the abundances of carbon, oxygen, nitrogen, phosphorus, sulfur, silicon, magnesium, and iron. Our analysis leads to several predictions for which habitability criteria are correct by determining which ones make our observations of the physical constants, as well as a few other observed features of our universe, most likely. Our results indicate that carbon-rich or carbon-poor planets are uninhabitable, slightly magnesium-rich planets are habitable, and life does not depend on nitrogen abundance too sensitively. We also find suggestive but inconclusive evidence that metal-rich planets and phosphorus-poor planets are habitable. These predictions can then be checked by probing regions of our universe that closely resemble normal environments in other universes. If any of these predictions are found to be wrong, the multiverse scenario would predict that the majority of observers are born in universes differing substantially from ours, and so can be ruled out, to varying degrees of statistical significance." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "af1-universe-08-00651", + "affPubRaw": "Blue Marble Space Institute of Science, Seattle, WA 98154, USA" + } + ], + "attrib": { + "email": "mccullen@bmsis.org" + }, + "name": { + "given_name": "McCullen", + "surname": "Sandora" + } + }, + { + "affiliation": [ + { + "affPubID": "af2-universe-08-00651", + "affPubRaw": "Sellers Exoplanetary Environments Collaboration, NASA Goddard Space Flight Center, Greenbelt, MD 20771, USA" + }, + { + "affPubID": "af3-universe-08-00651", + "affPubRaw": "Department of Physics, American University, Washington, DC 20016, USA" + } + ], + "name": { + "given_name": "Vladimir", + "surname": "Airapetian" + } + }, + { + "affiliation": [ + { + "affPubID": "af4-universe-08-00651", + "affPubRaw": "School of Science, Western Sydney University, Locked Bag 1797, Penrith South Dc, NSW 2751, Australia" + } + ], + "name": { + "given_name": "Luke", + "surname": "Barnes" + } + }, + { + "affiliation": [ + { + "affPubID": "af5-universe-08-00651", + "affPubRaw": "Sydney Institute for Astronomy, School of Physics, A28, The University of Sydney, NSW 2006, Australia" + } + ], + "name": { + "given_name": "Geraint F.", + "surname": "Lewis" + } + }, + { + "affiliation": [ + { + "affPubID": "af6-universe-08-00651", + "affPubRaw": "Department of Earth and Environmental Science, University of Pennsylvania, Philadelphia, PA 19104, USA" + } + ], + "name": { + "given_name": "Ileana", + "surname": "P\u00e9rez-Rodr\u00edguez" + } + } + ], + "copyright": { + "statement": "\u00a9 2022 by the authors.", + "status": true + }, + "editorialHistory": { + "acceptedDate": "2022-12-05", + "receivedDates": [ + "2022-11-03" + ] + }, + "keywords": [ + { + "keyString": "multiverse", + "keySystem": "misc" + }, + { + "keyString": "habitability", + "keySystem": "misc" + }, + { + "keyString": "element abundances", + "keySystem": "misc" + } + ], + "openAccess": { + "license": "Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).", + "licenseURL": "https://creativecommons.org/licenses/by/4.0/", + "open": true + }, + "otherContributor": [ + { + "contrib": { + "name": { + "given_name": "Dirk", + "surname": "Schulze-Makuch" + } + }, + "role": "Academic Editor" + } + ], + "pagination": { + "electronicID": "651" + }, + "persistentIDs": [ + { + "DOI": "10.3390/universe8120651" + } + ], + "pubDate": { + "electrDate": "2022-12-07" + }, + "publication": { + "ISSN": [ + { + "issnString": "2218-1997", + "pubtype": "epub" + } + ], + "issueNum": "12", + "pubName": "Universe", + "pubYear": "2022", + "publisher": "MDPI", + "volumeNum": "8" + }, + "publisherIDs": [ + { + "Identifier": "universe-08-00651", + "attribute": "publisher-id" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + " Carter B. 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Astrophys. 1997 317 749 751 " + ], + "title": { + "textEnglish": "Multiverse Predictions for Habitability: Element Abundances" + } +} diff --git a/tests/stubdata/output/nlm_tf_gapfd_116_38.json b/tests/stubdata/output/nlm_tf_gapfd_116_38.json new file mode 100644 index 0000000..a113483 --- /dev/null +++ b/tests/stubdata/output/nlm_tf_gapfd_116_38.json @@ -0,0 +1,178 @@ +{ + "abstract": { + "textEnglish": "Eddy saturation describes the nonlinear mechanism in geophysical flows whereby, when average conditions are considered, direct forcing of the zonal flow increases the eddy kinetic energy, while the energy associated with the zonal flow does not increase. Here, we present a minimal baroclinic model that exhibits complete eddy saturation. Starting from Phillips' classical quasi-geostrophic two-level model on the beta channel of the mid-latitudes, we derive a reduced order model comprising of six ordinary differential equations including parameterised eddies. This model features two physically realisable steady state solutions, one a purely zonal flow and one where, additionally, finite eddy motions are present. As the baroclinic forcing in the form of diabatic heating is increased, the zonal solution loses stability and the eddy solution becomes attracting. After this bifurcation, the zonal components of the solution are independent of the baroclinic forcing, and the excess of heat in the low latitudes is efficiently transported northwards by finite eddies, in the spirit of baroclinic adjustment." + }, + "authors": [ + { + "affiliation": [ + { + "affPubID": "AF1", + "affPubRaw": "Department of Mathematics and Statistics, University of Reading, Reading, UK" + }, + { + "affPubID": "AF2", + "affPubRaw": "Centre for the Mathematics of Planet Earth, University of Reading, Reading, UK" + } + ], + "attrib": { + "email": "m.kobras@pgr.reading.ac.uk" + }, + "name": { + "given_name": "Melanie", + "surname": "Kobras" + } + }, + { + "affiliation": [ + { + "affPubID": "AF3", + "affPubRaw": "Department of Meteorology, University of Reading, Reading, UK" + } + ], + "name": { + "given_name": "Maarten H. P.", + "surname": "Ambaum" + } + }, + { + "affiliation": [ + { + "affPubID": "AF1", + "affPubRaw": "Department of Mathematics and Statistics, University of Reading, Reading, UK" + }, + { + "affPubID": "AF2", + "affPubRaw": "Centre for the Mathematics of Planet Earth, University of Reading, Reading, UK" + } + ], + "name": { + "given_name": "Valerio", + "surname": "Lucarini" + } + } + ], + "copyright": { + "statement": "\u00a9 2021 The Author(s). Published by Informa UK Limited, trading as Taylor & Francis Group", + "status": true + }, + "editorialHistory": { + "acceptedDate": "2021-10-05", + "receivedDates": [ + "2021-07-08" + ] + }, + "funding": [ + { + "agencyname": "Engineering and Physical Sciences Research Council", + "awardnumber": "EP/R513301/1" + }, + { + "agencyname": "EPSRC" + }, + { + "agencyname": "EU Horizon 2020", + "awardnumber": "820970" + } + ], + "keywords": [ + { + "keyString": "Eddy saturation", + "keySystem": "misc" + }, + { + "keyString": "baroclinic instability", + "keySystem": "misc" + }, + { + "keyString": "baroclinic adjustment", + "keySystem": "misc" + }, + { + "keyString": "Phillips' model", + "keySystem": "misc" + }, + { + "keyString": "frictional adjustment", + "keySystem": "misc" + } + ], + "openAccess": { + "license": "This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.", + "licenseURL": "http://creativecommons.org/licenses/by/4.0/", + "open": true + }, + "pagination": { + "firstPage": "38", + "lastPage": "55", + "pageCount": "18", + "pageRange": "38-55" + }, + "persistentIDs": [ + { + "DOI": "10.1080/03091929.2021.1990912" + } + ], + "pubDate": { + "printDate": "2022-01-02" + }, + "publication": { + "ISSN": [ + { + "issnString": "0309-1929", + "pubtype": "ppub" + }, + { + "issnString": "1029-0419", + "pubtype": "epub" + } + ], + "issueNum": "1", + "pubName": "Geophysical & Astrophysical Fluid Dynamics", + "pubYear": "2022", + "publisher": "Taylor & Francis", + "volumeNum": "116" + }, + "publisherIDs": [ + { + "Identifier": "1990912", + "attribute": "publisher-id" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "JATS", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + " Ambaum , M.H.P. and Novak , L. , A nonlinear oscillator describing storm track variability . 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" + ], + "title": { + "textEnglish": "Eddy saturation in a reduced two-level model of the atmosphere" + } +} diff --git a/tests/test_elsevier.py b/tests/test_elsevier.py index d224fab..a66b674 100644 --- a/tests/test_elsevier.py +++ b/tests/test_elsevier.py @@ -15,6 +15,7 @@ def setUp(self): stubdata_dir = os.path.join(os.path.dirname(__file__), "stubdata/") self.inputdir = os.path.join(stubdata_dir, "input") self.outputdir = os.path.join(stubdata_dir, "output") + self.maxDiff = None def test_elsevier(self): filenames = [ @@ -63,6 +64,4 @@ def test_elsevier(self): self.assertTrue(abs(time_difference) < datetime.timedelta(seconds=10)) parsed["recordData"]["parsedTime"] = "" - print(test_infile) - self.maxDiff = None self.assertEqual(parsed, output_data) diff --git a/tests/test_jats.py b/tests/test_jats.py index 94a2449..d257264 100644 --- a/tests/test_jats.py +++ b/tests/test_jats.py @@ -21,7 +21,10 @@ def setUp(self): def test_jats(self): filenames = [ + "jats_edp_jnwpu_40_96", + "jats_edp_aa_661_70", "jats_nature_41467_2023_Article_40261_nlm", + "jats_nature_natsd_12_7375", "jats_spie_jmnmm_1.JMM.21.4.041407", "jats_spie_spie_12.2663387", "jats_spie_spie_12.2665113", @@ -48,14 +51,18 @@ def test_jats(self): "jats_springer_JHEP_JHEP07_2023_200", "jats_springer_AcMSn_s10409-023-23108-x", "jats_springer_NatCo_s41467-023-40272-3", + "jats_springer_cldy_84_1543", + "jats_springer_jhep_2022_05_05", "jats_apj_859_2_101", "jats_mnras_493_1_141", "jats_aj_158_4_139", "jats_iop_ansnn_12_2_025001", "jats_aip_aipc_2470_040010", "jats_aip_amjph_90_286", + "jats_iop_jinst_17_05_P05009", "jats_phrvd_106_023001", "jats_pnas_1715554115", + "jats_pnas_119_2201344119", "jats_iop_no_contribs", "jats_iop_no_orcid_tag", "jats_iop_preprint_in_record", @@ -64,6 +71,12 @@ def test_jats(self): "jats_a+a_subtitle", "jats_iucr_d-60-02355", "jats_iucr_d-75-00616", + "jats_aps_phrvd_100_052015", + "jats_aps_phrvx_12_021031", + "mdpi_climate-11-00147", + "mdpi_galaxies-11-00090", + "mdpi_symmetry-15-00939", + "mdpi_universe-08-00651", ] for f in filenames: test_infile = os.path.join(self.inputdir, f + ".xml") @@ -98,6 +111,7 @@ def test_jats_lxml(self): # test parsing with BeautifulSoup parser='lxml' filenames = [ "jats_iop_aj_162_1", + "nlm_tf_gapfd_116_38", ] for f in filenames: test_infile = os.path.join(self.inputdir, f + ".xml") @@ -126,7 +140,6 @@ def test_jats_lxml(self): ) self.assertTrue(abs(time_difference) < datetime.timedelta(seconds=10)) parsed["recordData"]["parsedTime"] = "" - print(test_infile) self.assertEqual(parsed, output_data) @@ -172,5 +185,4 @@ def test_jats_cite_context(self): output_text = fp.read() output_data_tags = json.loads(output_text) cite_context = parser.citation_context(input_data, text_output=False) - print(test_infile) self.assertEqual(cite_context, output_data_tags) From 4f6e7bc44efe9bf30c9c26a195783ebf63a96b49 Mon Sep 17 00:00:00 2001 From: Matthew Templeton Date: Thu, 18 Apr 2024 16:20:46 -0400 Subject: [PATCH 05/10] Removing commented-out logging blocks from tests modified: tests/test_datacite.py modified: tests/test_wiley.py --- tests/test_datacite.py | 9 --------- tests/test_wiley.py | 9 --------- 2 files changed, 18 deletions(-) diff --git a/tests/test_datacite.py b/tests/test_datacite.py index c3faf52..3e44f47 100644 --- a/tests/test_datacite.py +++ b/tests/test_datacite.py @@ -7,15 +7,6 @@ from adsingestp.parsers import datacite -# import logging -# proj_dir = os.path.abspath(os.path.join(os.path.dirname(__file__), os.pardir, "adsingestp")) -# logging.basicConfig( -# format="%(levelname)s %(asctime)s %(message)s", -# filename=os.path.join(proj_dir, "logs", "parser.log"), -# level=logging.INFO, -# force=True, -# ) - TIMESTAMP_FMT = "%Y-%m-%dT%H:%M:%S.%fZ" diff --git a/tests/test_wiley.py b/tests/test_wiley.py index a9fbf14..6125d94 100644 --- a/tests/test_wiley.py +++ b/tests/test_wiley.py @@ -7,15 +7,6 @@ from adsingestp.parsers import wiley -# import logging -# proj_dir = os.path.abspath(os.path.join(os.path.dirname(__file__), os.pardir, "adsingestp")) -# logging.basicConfig( -# format="%(levelname)s %(asctime)s %(message)s", -# filename=os.path.join(proj_dir, "logs", "parser.log"), -# level=logging.INFO, -# force=True, -# ) - TIMESTAMP_FMT = "%Y-%m-%dT%H:%M:%S.%fZ" From 918b718b7f5028fbc3e1b913c20fb8fbf1a8357d Mon Sep 17 00:00:00 2001 From: Matthew Templeton Date: Fri, 26 Apr 2024 16:04:16 -0400 Subject: [PATCH 06/10] Fix for elsevier with nested author groups modified: adsingestp/parsers/elsevier.py new file: tests/stubdata/input/els_phlb_compound_affil.xml new file: tests/stubdata/output/els_phlb_compound_affil.json modified: tests/test_elsevier.py --- adsingestp/parsers/elsevier.py | 148 +- .../input/els_phlb_compound_affil.xml | 1 + .../output/els_phlb_compound_affil.json | 32126 ++++++++++++++++ tests/test_elsevier.py | 1 + 4 files changed, 32225 insertions(+), 51 deletions(-) create mode 100644 tests/stubdata/input/els_phlb_compound_affil.xml create mode 100644 tests/stubdata/output/els_phlb_compound_affil.json diff --git a/adsingestp/parsers/elsevier.py b/adsingestp/parsers/elsevier.py index 353fa03..4492e33 100644 --- a/adsingestp/parsers/elsevier.py +++ b/adsingestp/parsers/elsevier.py @@ -11,6 +11,27 @@ logger = logging.getLogger(__name__) +def flatten_author_groups(soup): + # takes a beautiful soup object as input + # recursively extracts author groups from it + # returning a list of flat author groups + # without any embedded groups + group_list = [] + ag = soup.find('ce:author-group').extract() + while ag.find('ce:author-group'): + group_list.append(flatten_author_groups(ag)) + g2 = [ag] + g2.extend(group_list) + group_list = [] + for g in g2: + if type(g) == list: + group_list.append(g[0]) + else: + group_list.append(g) + return group_list + + + class ElsevierParser(BaseBeautifulSoupParser): author_collaborations_params = {} @@ -236,60 +257,85 @@ def _parse_permissions(self): copyright_stub + " Elsevier Science B.V. All rights reserved." ) + def _parse_author_group(self, author_group): + # build affiliations cross-reference dict + group_author_list = [] + affs_xref = {} + + affs_xref_raw = author_group.find_all("ce:affiliation") + for aff in affs_xref_raw: + if aff.find("ce:label"): + label = aff.find("ce:label").get_text() + else: + label = "ALLAUTH" + if aff.find("ce:textfn"): + # formatted affiliation string + # note: sa:affiliation contains the parsed affiliation - not useful now but may be in the future + value = aff.find("ce:textfn").get_text() + elif aff.find("ce:source-text"): + # raw affiliation string + value = aff.find("ce:source-text").get_text() + else: + value = "" + if label == "ALLAUTH": + # collect all of the implicit affiliations in a list + value_list = affs_xref.get("ALLAUTH", []) + value_list.append(value) + affs_xref["ALLAUTH"] = value_list + else: + affs_xref[label] = value + + affs_footnotes_raw = author_group.find_all("ce:footnote") + for aff in affs_footnotes_raw: + if aff.find("ce:label"): + label = aff.find("ce:label").get_text() + else: + label = "ALLAUTH" + if aff.find("ce:note-para"): + value = aff.find("ce:note-para").get_text() + if label == "ALLAUTH": + # collect all of the implicit affiliations in a list + value_list = affs_xref.get("ALLAUTH", []) + value_list.append(value) + affs_xref["ALLAUTH"] = value_list + else: + affs_xref[label] = value + + authors_raw = author_group.find_all("ce:author") + for author in authors_raw: + author_tmp = {} + if author.find("ce:surname"): + if author.find("ce:given-name"): + author_tmp["given"] = author.find("ce:given-name").get_text() + author_tmp["surname"] = author.find("ce:surname").get_text() + elif author.find("ce:given-name") and not author.find("ce:surname"): + # In case given-name is present, but no surname is available, put the given name in the surname + author_tmp["surname"] = author.find("ce:given-name") + author_tmp["orcid"] = author.get("orcid", "") + if ( + author.find("ce:e-address") + and author.find("ce:e-address").get("type", "") == "email" + ): + author_tmp["email"] = author.find("ce:e-address").get_text() + if author.find("ce:cross-ref") and author.find("ce:cross-ref").find("sup"): + affs = [] + for i in author.find("ce:cross-ref").find_all("sup"): + aff_label = i.get_text() + # don't append an empty aff + if affs_xref.get(aff_label): + affs.append(affs_xref[aff_label]) + author_tmp["aff"] = affs + elif affs_xref.get("ALLAUTH"): + author_tmp["aff"] = affs_xref["ALLAUTH"] + group_author_list.append(author_tmp) + return group_author_list + def _parse_authors(self): author_list = [] if self.record_meta.find("ce:author-group"): - # build affiliations cross-reference dict - affs_xref_raw = self.record_meta.find("ce:author-group").find_all("ce:affiliation") - affs_xref = {} - for aff in affs_xref_raw: - if aff.find("ce:label"): - label = aff.find("ce:label").get_text() - else: - label = "ALLAUTH" - if aff.find("ce:textfn"): - # formatted affiliation string - # note: sa:affiliation contains the parsed affiliation - not useful now but may be in the future - value = aff.find("ce:textfn").get_text() - elif aff.find("ce:source-text"): - # raw affiliation string - value = aff.find("ce:source-text").get_text() - else: - value = "" - if label == "ALLAUTH": - # collect all of the implicit affiliations in a list - value_list = affs_xref.get("ALLAUTH", []) - value_list.append(value) - affs_xref["ALLAUTH"] = value_list - else: - affs_xref[label] = value - authors_raw = self.record_meta.find("ce:author-group").find_all("ce:author") - for author in authors_raw: - author_tmp = {} - if author.find("ce:surname"): - if author.find("ce:given-name"): - author_tmp["given"] = author.find("ce:given-name").get_text() - author_tmp["surname"] = author.find("ce:surname").get_text() - elif author.find("ce:given-name") and not author.find("ce:surname"): - # In case given-name is present, but no surname is available, put the given name in the surname - author_tmp["surname"] = author.find("ce:given-name") - author_tmp["orcid"] = author.get("orcid", "") - if ( - author.find("ce:e-address") - and author.find("ce:e-address").get("type", "") == "email" - ): - author_tmp["email"] = author.find("ce:e-address").get_text() - if author.find("ce:cross-ref") and author.find("ce:cross-ref").find("sup"): - affs = [] - for i in author.find("ce:cross-ref").find_all("sup"): - aff_label = i.get_text() - # don't append an empty aff - if affs_xref.get(aff_label): - affs.append(affs_xref[aff_label]) - author_tmp["aff"] = affs - elif affs_xref.get("ALLAUTH"): - author_tmp["aff"] = affs_xref["ALLAUTH"] - author_list.append(author_tmp) + author_groups = flatten_author_groups(self.record_meta) + for ag in author_groups: + author_list.extend(self._parse_author_group(ag)) elif self.record_header.find("dct:creator"): name_parser = utils.AuthorNames() authors_raw = self.record_header.find_all("dct:creator") diff --git a/tests/stubdata/input/els_phlb_compound_affil.xml b/tests/stubdata/input/els_phlb_compound_affil.xml new file mode 100644 index 0000000..5686580 --- /dev/null +++ b/tests/stubdata/input/els_phlb_compound_affil.xml @@ -0,0 +1 @@ +application/xmlSearch for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at [formula omitted]The CMS CollaborationA. HayrapetyanA. TumasyanW. AdamJ.W. AndrejkovicT. BergauerS. ChatterjeeK. DamanakisM. DragicevicP.S. HussainM. JeitlerN. KrammerA. LiD. LikoI. MikulecJ. SchieckR. SchöfbeckD. SchwarzM. SonawaneS. TemplW. WaltenbergerC.-E. WulzM.R. DarwishT. JanssenP. Van MechelenE.S. BolsJ. D'HondtS. DansanaA. De MoorM. DelcourtH. El FahamS. LowetteI. MakarenkoD. MüllerA.R. SahasransuS. TavernierM. TytgatS. Van PutteD. VanneromB. ClerbauxG. De LentdeckerL. FavartD. HohovJ. JaramilloA. KhalilzadehK. LeeM. MahdavikhorramiA. MalaraS. ParedesL. PétréN. PostiauL. ThomasM. Vanden BemdenC. Vander VeldeP. VanlaerM. De CoenD. DoburY. HongJ. KnolleL. LambrechtG. MestdachC. RendónA. SamalanK. SkovpenN. Van Den BosscheJ. van der LindenL. WezenbeekA. BeneckeG. BrunoC. CaputoC. DelaereI.S. DonertasA. GiammancoK. JaffelSa. JainV. LemaitreJ. LidrychP. MastrapasquaK. MondalT.T. TranS. WertzG.A. AlvesE. CoelhoC. HenselT. Menezes De OliveiraA. MoraesP. Rebello TelesM. SoeiroW.L. Aldá JúniorM. Alves Gallo PereiraM. Barroso Ferreira FilhoH. Brandao MalbouissonW. CarvalhoJ. ChinellatoE.M. Da CostaG.G. Da SilveiraD. De Jesus DamiaoS. Fonseca De SouzaJ. MartinsC. Mora HerreraK. Mota AmariloL. MundimH. NogimaA. SantoroA. SznajderM. ThielA. Vilela PereiraC.A. BernardesL. CalligarisT.R. Fernandez Perez TomeiE.M. GregoresP.G. MercadanteS.F. NovaesB. OrzariSandra S. PadulaA. AleksandrovG. AntchevR. HadjiiskaP. IaydjievM. MishevaM. ShopovaG. SultanovA. DimitrovL. LitovB. PavlovP. PetkovA. PetrovE. ShumkaS. KeshriS. ThakurT. ChengQ. GuoT. JavaidL. YuanZ. HuJ. LiuK. YiG.M. ChenH.S. ChenM. ChenF. IemmiC.H. JiangA. KapoorH. LiaoZ.-A. LiuR. SharmaJ.N. SongJ. TaoC. WangJ. WangZ. WangH. ZhangA. AgapitosY. BanA. LevinC. LiQ. LiY. MaoS.J. QianX. SunD. WangH. YangL. ZhangC. ZhouZ. YouN. LuG. BauerX. GaoD. LeggatH. OkawaY. ZhangZ. LinC. LuM. XiaoC. AvilaD.A. Barbosa TrujilloA. CabreraC. FlorezJ. FragaJ.A. Reyes VegaJ. Mejia GuisaoF. RamirezM. RodriguezJ.D. Ruiz AlvarezD. GiljanovicN. GodinovicD. LelasA. SculacM. KovacT. SculacP. BargassaV. BrigljevicB.K. ChitrodaD. FerencekS. MishraA. StarodumovT. SusaA. AttikisK. ChristoforouS. KonstantinouJ. MousaC. NicolaouF. PtochosP.A. RazisH. RykaczewskiH. SakaA. StepennovM. FingerM. Finger Jr.A. KvetonE. AyalaE. Carrera JarrinH. AbdallaY. AssranM.A. MahmoudY. MohammedR.K. DewanjeeK. EhatahtM. KadastikT. LangeS. NandanC. NielsenJ. PataM. RaidalL. TaniC. VeelkenH. KirschenmannK. OsterbergM. VoutilainenS. BharthuarE. BrückenF. GarciaJ. HavukainenK.T.S. KallonenR. KinnunenT. LampénK. Lassila-PeriniS. LehtiT. LindénM. LottiL. MartikainenM. MyllymäkiM.m. RantanenH. SiikonenE. TuominenJ. TuominiemiP. LuukkaH. PetrowT. TuuvaM. BesanconF. CoudercM. DejardinD. DenegriJ.L. FaureF. FerriS. GanjourP. GrasG. Hamel de MonchenaultV. LohezicJ. MalclesJ. RanderA. RosowskyM.Ö. SahinA. Savoy-NavarroP. SimkinaM. TitovM. TornagoC. Baldenegro BarreraF. BeaudetteA. Buchot PerraguinP. BussonA. CappatiC. CharlotF. DamasO. DavignonA. De WitG. FalmagneB.A. Fontana Santos AlvesS. GhoshA. GilbertR. Granier de CassagnacA. HakimiB. HarikrishnanL. KalipolitiG. LiuJ. MottaM. NguyenC. OchandoL. PortalesR. SalernoJ.B. SauvanY. SiroisA. TarabiniE. VernazzaA. ZabiA. ZghicheJ.-L. AgramJ. AndreaD. ApparuD. BlochJ.-M. BromE.C. ChabertC. CollardS. FalkeU. GoerlachC. GrimaultR. HaeberleA.-C. Le BihanM. MeenaG. SahaM.A. SessiniP. Van HoveS. BeauceronB. BlanconG. BoudoulN. ChanonJ. ChoiD. ContardoP. DepasseC. DozenH. El MamouniJ. FayS. GasconM. GouzevitchC. GreenbergG. GrenierB. IlleI.B. LaktinehM. LethuillierL. MirabitoS. PerriesA. PurohitM. Vander DoncktP. VerdierJ. XiaoA. KhvedelidzeI. LomidzeZ. TsamalaidzeV. BottaL. FeldK. KleinM. LipinskiD. MeuserA. PaulsN. RöwertM. TeroerdeS. DiekmannA. DodonovaN. EichD. EliseevF. EngelkeM. ErdmannP. FackeldeyB. FischerT. HebbekerK. HoepfnerF. IvoneA. JungM.y. LeeL. MastrolorenzoF. MausolfM. MerschmeyerA. MeyerS. MukherjeeD. NollA. NovakF. NowotnyA. PozdnyakovY. RathW. RedjebF. RehmH. ReithlerU. SarkarV. SarkisoviA. SchmidtA. SharmaJ.L. SpahA. SteinF. Torres Da Silva De AraujoL. VigilanteS. WiedenbeckS. ZaleskiC. DziwokG. FlüggeW. Haj AhmadT. KressA. NowackO. PoothA. StahlT. ZiemonsA. ZotzH. Aarup PetersenM. Aldaya MartinJ. AlimenaS. AmorosoY. AnS. BaxterM. BayatmakouH. Becerril GonzalezO. BehnkeA. BelvedereS. BhattacharyaF. BlekmanK. BorrasD. BrunnerA. CampbellA. CardiniC. ChengF. ColombinaS. Consuegra RodríguezG. Correia SilvaM. De SilvaG. EckerlinD. EcksteinL.I. Estevez BanosO. FilatovE. GalloA. GeiserA. GiraldiG. GreauV. GuglielmiM. GuthoffA. HinzmannA. JafariL. JeppeN.Z. JomhariB. KaechM. KasemannH. KavehC. KleinwortR. KoglerM. KommD. KrückerW. LangeD. Leyva PerniaK. LipkaW. LohmannR. MankelI.-A. Melzer-PellmannM. Mendizabal MorentinJ. MetwallyA.B. MeyerG. MilellaA. MussgillerL.P. NairA. NürnbergY. OtaridJ. ParkD. Pérez AdánE. RankenA. RasperezaB. Ribeiro LopesJ. RübenachA. SaggioM. SchamS. SchnakeP. SchützeC. SchwanenbergerD. SelivanovaM. ShchedrolosievR.E. Sosa RicardoD. StaffordF. VazzolerA. Ventura BarrosoR. 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ZygalaA. BasnetB. BylsmaM. CarriganL.S. DurkinC. HillM. JoyceM. Nunez OrnelasK. WeiB.L. WinerB.R. YatesF.M. AddesaH. BouchamaouiP. DasG. DezoortP. ElmerA. FrankenthalB. GreenbergN. HaubrichG. KoppS. KwanD. LangeA. LoeligerD. MarlowI. OjalvoJ. OlsenA. ShevelevD. SticklandC. TullyS. MalikA.S. BakshiV.E. BarnesS. ChandraR. ChawlaS. DasA. GuL. GutayM. JonesA.W. JungD. KondratyevA.M. KoshyM. LiuG. NegroN. NeumeisterG. PaspalakiS. PiperovV. ScheurerJ.F. SchulteM. StojanovicJ. ThiemanA.K. VirdiF. WangW. XieJ. DolenN. ParasharA. PathakD. AcostaT. CarnahanK.M. EcklundP.J. Fernández MantecaS. FreedP. GardnerF.J.M. GeurtsW. LiO. Miguel ColinB.P. PadleyR. RedjimiJ. RotterE. YigitbasiY. ZhangA. BodekP. de BarbaroR. DeminaJ.L. DulembaC. FallonA. Garcia-BellidoO. HindrichsA. KhukhunaishviliN. ParmarP. ParyginE. PopovaR. TausG.P. Van OnsemK. GoulianosB. ChiaritoJ.P. ChouY. GershteinE. HalkiadakisA. HartM. HeindlD. JaroslawskiO. KarachebanI. LaflotteA. LathR. MontalvoK. NashH. RoutrayS. SalurS. SchnetzerS. SomalwarR. StoneS.A. ThayilS. ThomasJ. VoraH. WangH. AcharyaD. AllyA.G. DelannoyS. FiorendiS. HigginbothamT. HolmesA.R. KanugantiN. KarunarathnaL. LeeE. NibigiraS. SpanierD. AebiM. AhmadO. BouhaliM. DalchenkoR. EusebiJ. GilmoreT. HuangT. KamonH. KimS. LuoS. MalhotraR. MuellerD. OvertonD. RathjensA. SafonovN. AkchurinJ. DamgovV. HegdeA. HussainY. KazhykarimK. LamichhaneS.W. LeeA. MankelT. PeltolaI. VolobouevA. WhitbeckE. AppeltS. GreeneA. GurrolaW. JohnsR. Kunnawalkam ElayavalliA. MeloF. RomeoP. SheldonS. TuoJ. VelkovskaJ. ViinikainenB. CardwellB. CoxJ. HakalaR. HiroskyA. LedovskoyC. NeuC.E. Perez LaraP.E. KarchinA. AravindS. BanerjeeK. BlackT. BoseS. DasuI. De BruynP. EveraertsC. GalloniH. HeM. HerndonA. HerveC.K. KorakaA. LanaroR. LovelessJ. Madhusudanan SreekalaA. MallampalliA. MohammadiS. MondalG. ParidaD. PinnaA. SavinV. ShangV. SharmaW.H. SmithD. TeagueH.F. TsoiW. VetensA. WardenS. AfanasievV. AndreevYu. AndreevT. AushevM. AzarkinA. BabaevA. BelyaevV. BlinovE. BoosV. BorshchD. BudkouskiV. BunichevV. ChekhovskyR. ChistovM. DanilovA. DermenevT. DimovaD. DruzhkinM. DubininL. DudkoA. ErshovG. GavrilovV. GavrilovS. GninenkoV. GolovtcovN. GolubevI. GolutvinI. GorbunovA. GribushinY. IvanovV. KachanovV. KarjavineA. KarneyeuV. KimM. KirakosyanD. KirpichnikovM. KirsanovV. KlyukhinV. KorenkovA. KozyrevN. KrasnikovA. LanevP. LevchenkoN. LychkovskayaV. MakarenkoA. MalakhovV. MatveevV. MurzinA. NikitenkoS. ObraztsovV. OreshkinV. PalichikV. PerelyginM. PerfilovS. PolikarpovV. PopovO. RadchenkoM. SavinaV. SavrinV. ShalaevS. ShmatovS. ShulhaY. SkovpenS. SlabospitskiiV. SmirnovD. SosnovV. SulimovE. TcherniaevA. TerkulovO. TeryaevI. TlisovaA. ToropinL. UvarovA. UzunianP. VolkovA. VorobyevG. VorotnikovN. VoytishinB.S. YuldashevA. ZarubinI. ZhizhinA. ZhokinCMSTop quarksExtra Higgs bosonYukawa couplingsPhysics Letters B 850 (2024). doi:10.1016/j.physletb.2024.138478journalPhysics Letters B© 2024 The Author(s). Published by Elsevier B.V. Funded by SCOAP³.Elsevier B.V.0370-2693850March 202410.1016/j.physletb.2024.138478http://dx.doi.org/10.1016/j.physletb.2024.138478doi:10.1016/j.physletb.2024.138478138478http://vtw.elsevier.com/data/voc/oa/OpenAccessStatus#Full2024-01-12T00:06:30ZSCOAP³ - Sponsoring Consortium for Open Access Publishing in Particle Physicshttp://vtw.elsevier.com/data/voc/oa/SponsorType#FundingBodyhttp://creativecommons.org/licenses/by/4.0/2024-02-02T00:00:00.000Z2024-02-09T00:00:00.000ZThis is an open access article under the CC BY license.JournalsS300.3PLB138478138478S0370-2693(24)00017-010.1016/j.physletb.2024.138478The Author(s)ExperimentsCMSdata preservation, re-use and open access policyFig. 1Representative Feynman diagram for ttq‾ (q = u, c) production through a new scalar (H) or pseudoscalar (A) Higgs boson. In this analysis, events with q = q′ are considered.Fig. 1Fig. 2The pre-fit CvsL (upper) and CvsB (lower) distributions for the selected highest pT jet. The predictions for mA = 350 GeV with A-H interference assuming mA − mH = 50 GeV for ρtu = 1.0 (solid red line) and ρtc = 1.0 (dashed red line) are also displayed. The numbers in square brackets represent the yields for each sample. The uncertainty bars on the points and the hatched bands represent the statistical uncertainties in the data and in the background predictions, respectively. Beneath each plot the ratio of data to predictions is shown. The uncertainty bars in the ratio plots include statistical uncertainties in the data and in the background predictions.Fig. 2Fig. 3Post-fit distributions of the BDT discriminants combining the categories e±e±, μ±μ±, and e±μ±, and all data-taking periods, for mA = 350 GeV with ρtu = 1.0 (upper), and ρtc = 1.0 (lower) with the A-H interference. The numbers in square brackets represent the yields for each sample. The uncertainty bars on the points represent the statistical uncertainties in the data. Beneath each plot the ratio of data to predictions is shown. The uncertainty bars in the ratio plots include statistical uncertainties in the data and the total uncertainty in the background predictions, and the hatched bands represent the total uncertainty in the background predictions.Fig. 3Fig. 4Observed and expected 95% CL upper limits on the signal strength as functions of mA for g2HDM using different coupling assumptions: ρtu = 0.1, 0.4, 1.0 (upper) and ρtc = 0.1, 0.4, 1.0 (lower) without interference, for the combination of the e±e±, μ±μ±, and e±μ± categories and all data-taking periods. The inner (green) band and the outer (yellow) band indicate the regions containing 68 and 95%, respectively, of the distribution of limits expected under the background-only hypothesis.Fig. 4Fig. 5Observed and expected 95% CL upper limits on the signal strength as functions of mA for g2HDM using different coupling assumptions: ρtu = 0.1, 0.4, 1.0 (upper) and ρtc = 0.1, 0.4, 1.0 (lower) with A-H interference assuming mA − mH = 50 GeV, for the combination of the e±e±, μ±μ±, and e±μ± categories and all data-taking periods. The inner (green) band and the outer (yellow) band indicate the regions containing 68 and 95%, respectively, of the distribution of limits expected under the background-only hypothesis.Fig. 5Fig. 6Observed 95% CL upper limit on the signal strength as a function of mA and ρtu (upper) and ρtc (lower) for g2HDM without the A-H interference, for the combination of the e±e±, μ±μ±, and e±μ± categories. The color axis represents the observed upper limit on the signal strength. Expected (dashed lines) and observed (solid lines) exclusion contours are also shown.Fig. 6Fig. 7Observed 95% CL upper limit on the signal strength as a function of mA and ρtu (upper) and ρtc (lower) for g2HDM signal model with the A-H interference, for the combination of the e±e±, μ±μ±, and e±μ± categories. The color axis represents the observed upper limit on the signal strength. Expected (dashed lines) and observed (solid lines) exclusion contours are also shown.Fig. 7Table 1Input variables of the BDT. Jets and leptons are ordered by pT.Table 1Input variables of the BDTCvsL(ja)a = 1,2,3Charm- vs light-quark jet identification variableCvsB(ja)a = 1,2,3Charm- vs bottom-quark jet identification variableΔR(ja,jb)1 ≤ a < b ≤ 3Angular separation between jetsm(ja,jb)1 ≤ a < b ≤ 3Invariant mass of jet pairsΔR(ja,lb)a = 1,2,3; b = 1,2Angular separation between jet and leptonm(ja,lb)a = 1,2,3; b = 1,2Invariant mass of jet-lepton pairspT(ℓa)a = 1,2Transverse momentum of leptonsm(ℓ1,ℓ2,ja)a = 1,2,3Invariant mass of the two leptons plus the highest pT jetm(ℓ1,ℓ2)Invariant mass of the two leptonsHTScalar pT sum of the jetspTmissMissing transverse momentumTable 2Summary of systematic uncertainties for ρtc = 0.4 and mA = 350 GeV with A-H interference assuming mA − mH = 50 GeV. The first column indicates the source of uncertainty. The second column specifies whether the shape of the fit discriminant is affected by the nuisance parameter (✓) or not (dash). The impact in percent of these nuisance parameters on the pre-fit expected event yields is displayed in the third column. This column is subdivided into three event categories representing the analysis channels. The percentage impacts are given as a range of values representing the minimum and maximum differences obtained in the different bins of the BDT distribution through the four data-taking periods. The numbers for the normalization component of the nonprompt lepton background represent the uncertainties used for each data-taking period. Whether or not a nuisance parameter is taken correlated across years and categories is specified in the last two columns. The luminosity and jet flavor identification nuisances are only partially correlated across years.Table 2Uncertainty sourceShapeCategoryCorrelated acrosse±e±μ±μ±e±μ±YearsCategoriesExperimentalLuminosity—1.2–2.51.2–2.51.2–2.5✓✓Pileup✓<0.1–2.8<0.1–1.8<0.1–2.3✓✓Trigger efficiency✓0.4–2.60.2–1.10.3–1.2——L1 trigger inefficiency✓0.1–0.80.1–0.30.1–0.4✓✓Lepton identification✓0.1–1.7<0.1–0.4<0.1–0.6—✓Lepton energy scale✓—<0.1–0.2<0.1–0.2—✓Charge misid.✓1.2–13.1————Jet energy scale✓<0.1–4.5<0.1–1.7<0.1–1.5✓✓Jet energy resolution✓<0.1–2.6<0.1–1.8<0.1–1.6—✓Unclustered energy✓<0.1–2.6<0.1–0.5<0.1–0.8—✓Jet flavor identification✓<0.1–12.1<0.1–8.8<0.1–11.6✓✓Nonprompt lepton BGstatistical component✓<0.1–27.21.9–16.23.0–13.2—✓Nonprompt lepton BG—27,15,11,1027,15,11,1027,15,11,10—✓TheoreticalSignal QCD scales✓10.3–10.510.0–10.29.9–10.0✓✓Signal PDF✓0.70.6–0.70.5–0.6✓✓Signal parton shower✓3.6–4.34.0–4.36.3–7.3✓✓tt‾—6.16.16.1✓✓VV—4.54.54.5✓✓VBS—10.410.410.4✓✓tt‾H—7.87.87.8✓✓tt‾W—10.710.710.7✓✓Other backgrounds—5.45.45.4✓✓Table 3Observed (expected) lower limits on mA at 95% CL. For the scenario without interference, the limits on mH and mA are the same.Table 3Observed (expected) mass limit [GeV]withoutwithwithinterferenceinterferenceinterferencemA or mHmAmHρtu0.4920 (920)1000 (1000)950 (950)1.01000 (1000)1000 (1000)950 (950)ρtc0.4no limit340 (370)290 (320)1.0770 (680)810 (670)760 (620)LetterSearch for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at s=13TeVThe CMS Collaboration⋆A.HayrapetyanA.Tumasyan1Yerevan Physics Institute, Yerevan, ArmeniaYerevan Physics InstituteYerevanArmeniaYerevan Physics Institute, Yerevan, Armenia1Also at Yerevan State University, Yerevan, Armenia.W.AdamJ.W.AndrejkovicT.BergauerS.ChatterjeeK.DamanakisM.DragicevicP.S.HussainM.Jeitler2N.KrammerA.LiD.LikoI.MikulecJ.Schieck2R.SchöfbeckD.SchwarzM.SonawaneS.TemplW.WaltenbergerC.-E.Wulz2Institut für Hochenergiephysik, Vienna, AustriaInstitut für HochenergiephysikViennaAustriaInstitut für Hochenergiephysik, Vienna, Austria2Also at TU Wien, Vienna, Austria.M.R.Darwish3T.JanssenP.Van MechelenUniversiteit Antwerpen, Antwerpen, BelgiumUniversiteit AntwerpenAntwerpenBelgiumUniversiteit Antwerpen, Antwerpen, Belgium3Also at Institute of Basic and Applied Sciences, Faculty of Engineering, Arab Academy for Science, Technology and Maritime Transport, Alexandria, Egypt.E.S.BolsJ.D'HondtS.DansanaA.De MoorM.DelcourtH.El FahamS.LowetteI.MakarenkoD.MüllerA.R.SahasransuS.TavernierM.Tytgat4S.Van PutteD.VanneromVrije Universiteit Brussel, Brussel, BelgiumVrije Universiteit BrusselBrusselBelgiumVrije Universiteit Brussel, Brussel, Belgium4Also at Ghent University, Ghent, Belgium.B.ClerbauxG.De LentdeckerL.FavartD.HohovJ.JaramilloA.KhalilzadehK.LeeM.MahdavikhorramiA.MalaraS.ParedesL.PétréN.PostiauL.ThomasM.Vanden BemdenC.Vander VeldeP.VanlaerUniversité Libre de Bruxelles, Bruxelles, BelgiumUniversité Libre de BruxellesBruxellesBelgiumUniversité Libre de Bruxelles, Bruxelles, BelgiumM.De CoenD.DoburY.HongJ.KnolleL.LambrechtG.MestdachC.RendónA.SamalanK.SkovpenN.Van Den BosscheJ.van der LindenL.WezenbeekGhent University, Ghent, BelgiumGhent UniversityGhentBelgiumGhent University, Ghent, BelgiumA.BeneckeG.BrunoC.CaputoC.DelaereI.S.DonertasA.GiammancoK.JaffelSa.JainV.LemaitreJ.LidrychP.MastrapasquaK.MondalT.T.TranS.WertzUniversité Catholique de Louvain, Louvain-la-Neuve, BelgiumUniversité Catholique de LouvainLouvain-la-NeuveBelgiumUniversité Catholique de Louvain, Louvain-la-Neuve, BelgiumG.A.AlvesE.CoelhoC.HenselT.Menezes De OliveiraA.MoraesP.Rebello TelesM.SoeiroCentro Brasileiro de Pesquisas Fisicas, Rio de Janeiro, BrazilCentro Brasileiro de Pesquisas FisicasRio de JaneiroBrazilCentro Brasileiro de Pesquisas Fisicas, Rio de Janeiro, BrazilW.L.Aldá JúniorM.Alves Gallo PereiraM.Barroso Ferreira FilhoH.Brandao MalbouissonW.CarvalhoJ.Chinellato5E.M.Da CostaG.G.Da Silveira6D.De Jesus DamiaoS.Fonseca De SouzaJ.Martins7C.Mora HerreraK.Mota AmariloL.MundimH.NogimaA.SantoroA.SznajderM.ThielA.Vilela PereiraUniversidade do Estado do Rio de Janeiro, Rio de Janeiro, BrazilUniversidade do Estado do Rio de JaneiroRio de JaneiroBrazilUniversidade do Estado do Rio de Janeiro, Rio de Janeiro, Brazil5Also at Universidade Estadual de Campinas, Campinas, Brazil.6Also at Federal University of Rio Grande do Sul, Porto Alegre, Brazil.7Also at UFMS, Nova Andradina, Brazil.C.A.Bernardes6L.CalligarisT.R.Fernandez Perez TomeiE.M.GregoresP.G.MercadanteS.F.NovaesB.OrzariSandra S.PadulaUniversidade Estadual Paulista, Universidade Federal do ABC, São Paulo, BrazilUniversidade Estadual PaulistaUniversidade Federal do ABCSão PauloBrazilUniversidade Estadual Paulista, Universidade Federal do ABC, São Paulo, BrazilA.AleksandrovG.AntchevR.HadjiiskaP.IaydjievM.MishevaM.ShopovaG.SultanovInstitute for Nuclear Research and Nuclear Energy, Bulgarian Academy of Sciences, Sofia, BulgariaInstitute for Nuclear Research and Nuclear EnergyBulgarian Academy of SciencesSofiaBulgariaInstitute for Nuclear Research and Nuclear Energy, Bulgarian Academy of Sciences, Sofia, BulgariaA.DimitrovL.LitovB.PavlovP.PetkovA.PetrovE.ShumkaUniversity of Sofia, Sofia, BulgariaUniversity of SofiaSofiaBulgariaUniversity of Sofia, Sofia, BulgariaS.KeshriS.ThakurInstituto De Alta Investigación, Universidad de Tarapacá, Casilla 7 D, Arica, ChileInstituto De Alta InvestigaciónUniversidad de TarapacáCasilla 7 DAricaChileInstituto De Alta Investigación, Universidad de Tarapacá, Casilla 7 D, Arica, ChileT.ChengQ.GuoT.JavaidL.YuanBeihang University, Beijing, ChinaBeihang UniversityBeijingChinaBeihang University, Beijing, ChinaZ.HuJ.LiuK.Yi89Department of Physics, Tsinghua University, Beijing, ChinaDepartment of PhysicsTsinghua UniversityBeijingChinaDepartment of Physics, Tsinghua University, Beijing, China8Also at Nanjing Normal University, Nanjing, China.9Now at The University of Iowa, Iowa City, Iowa, USA.G.M.Chen10H.S.Chen10M.Chen10F.IemmiC.H.JiangA.Kapoor11H.LiaoZ.-A.Liu12R.Sharma13J.N.Song12J.TaoC.Wang10J.WangZ.Wang10H.ZhangInstitute of High Energy Physics, Beijing, ChinaInstitute of High Energy PhysicsBeijingChinaInstitute of High Energy Physics, Beijing, China10Also at University of Chinese Academy of Sciences, Beijing, China.11Also at China Center of Advanced Science and Technology, Beijing, China.12Also at University of Chinese Academy of Sciences, Beijing, China.13Also at China Spallation Neutron Source, Guangdong, China.A.AgapitosY.BanA.LevinC.LiQ.LiY.MaoS.J.QianX.SunD.WangH.YangL.ZhangC.ZhouState Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, ChinaState Key Laboratory of Nuclear Physics and TechnologyPeking UniversityBeijingChinaState Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, ChinaZ.YouSun Yat-Sen University, Guangzhou, ChinaSun Yat-Sen UniversityGuangzhouChinaSun Yat-Sen University, Guangzhou, ChinaN.LuUniversity of Science and Technology of China, Hefei, ChinaUniversity of Science and Technology of ChinaHefeiChinaUniversity of Science and Technology of China, Hefei, ChinaG.Bauer14Nanjing Normal University, Nanjing, ChinaNanjing Normal UniversityNanjingChinaNanjing Normal University, Nanjing, China14Now at Henan Normal University, Xinxiang, China.X.Gao15D.LeggatH.OkawaY.ZhangInstitute of Modern Physics and Key Laboratory of Nuclear Physics and Ion-beam Application (MOE) - Fudan University, Shanghai, ChinaInstitute of Modern PhysicsKey Laboratory of Nuclear PhysicsIon-beam Application (MOE)Fudan UniversityShanghaiChinaInstitute of Modern Physics and Key Laboratory of Nuclear Physics and Ion-beam Application (MOE) - Fudan University, Shanghai, China15Also at Université Libre de Bruxelles, Bruxelles, Belgium.Z.LinC.LuM.XiaoZhejiang University, Hangzhou, Zhejiang, ChinaZhejiang UniversityHangzhouZhejiangChinaZhejiang University, Hangzhou, Zhejiang, ChinaC.AvilaD.A.Barbosa TrujilloA.CabreraC.FlorezJ.FragaJ.A.Reyes VegaUniversidad de Los Andes, Bogota, ColombiaUniversidad de Los AndesBogotaColombiaUniversidad de Los Andes, Bogota, ColombiaJ.Mejia GuisaoF.RamirezM.RodriguezJ.D.Ruiz AlvarezUniversidad de Antioquia, Medellin, ColombiaUniversidad de AntioquiaMedellinColombiaUniversidad de Antioquia, Medellin, ColombiaD.GiljanovicN.GodinovicD.LelasA.SculacUniversity of Split, Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, Split, CroatiaUniversity of SplitFaculty of Electrical Engineering, Mechanical Engineering and Naval ArchitectureSplitCroatiaUniversity of Split, Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, Split, CroatiaM.KovacT.Sculac16University of Split, Faculty of Science, Split, CroatiaUniversity of SplitFaculty of ScienceSplitCroatiaUniversity of Split, Faculty of Science, Split, Croatia16Also at University of Latvia (LU), Riga, Latvia.P.BargassaV.BrigljevicB.K.ChitrodaD.FerencekS.MishraA.Starodumov17T.SusaInstitute Rudjer Boskovic, Zagreb, CroatiaInstitute Rudjer BoskovicZagrebCroatiaInstitute Rudjer Boskovic, Zagreb, Croatia17Also at an institute or an international laboratory covered by a cooperation agreement with CERN.A.AttikisK.ChristoforouS.KonstantinouJ.MousaC.NicolaouF.PtochosP.A.RazisH.RykaczewskiH.SakaA.StepennovUniversity of Cyprus, Nicosia, CyprusUniversity of CyprusNicosiaCyprusUniversity of Cyprus, Nicosia, CyprusM.FingerM.FingerJr.A.KvetonCharles University, Prague, Czech RepublicCharles UniversityPragueCzech RepublicCharles University, Prague, Czech RepublicE.AyalaEscuela Politecnica Nacional, Quito, EcuadorEscuela Politecnica NacionalQuitoEcuadorEscuela Politecnica Nacional, Quito, EcuadorE.Carrera JarrinUniversidad San Francisco de Quito, Quito, EcuadorUniversidad San Francisco de QuitoQuitoEcuadorUniversidad San Francisco de Quito, Quito, EcuadorH.Abdalla18Y.Assran1920Academy of Scientific Research and Technology of the Arab Republic of Egypt, Egyptian Network of High Energy Physics, Cairo, EgyptAcademy of Scientific Research and Technology of the Arab Republic of EgyptEgyptian Network of High Energy PhysicsCairoEgyptAcademy of Scientific Research and Technology of the Arab Republic of Egypt, Egyptian Network of High Energy Physics, Cairo, Egypt18Also at Cairo University, Cairo, Egypt.19Also at Suez University, Suez, Egypt.20Now at British University in Egypt, Cairo, Egypt.M.A.MahmoudY.MohammedCenter for High Energy Physics (CHEP-FU), Fayoum University, El-Fayoum, EgyptCenter for High Energy Physics (CHEP-FU)Fayoum UniversityEl-FayoumEgyptCenter for High Energy Physics (CHEP-FU), Fayoum University, El-Fayoum, EgyptR.K.Dewanjee21K.EhatahtM.KadastikT.LangeS.NandanC.NielsenJ.PataM.RaidalL.TaniC.VeelkenNational Institute of Chemical Physics and Biophysics, Tallinn, EstoniaNational Institute of Chemical Physics and BiophysicsTallinnEstoniaNational Institute of Chemical Physics and Biophysics, Tallinn, Estonia21Also at Birla Institute of Technology, Mesra, Mesra, India.H.KirschenmannK.OsterbergM.VoutilainenDepartment of Physics, University of Helsinki, Helsinki, FinlandDepartment of PhysicsUniversity of HelsinkiHelsinkiFinlandDepartment of Physics, University of Helsinki, Helsinki, FinlandS.BharthuarE.BrückenF.GarciaJ.HavukainenK.T.S.KallonenR.KinnunenT.LampénK.Lassila-PeriniS.LehtiT.LindénM.LottiL.MartikainenM.MyllymäkiM.m.RantanenH.SiikonenE.TuominenJ.TuominiemiHelsinki Institute of Physics, Helsinki, FinlandHelsinki Institute of PhysicsHelsinkiFinlandHelsinki Institute of Physics, Helsinki, FinlandP.LuukkaH.PetrowT.Tuuva†Lappeenranta-Lahti University of Technology, Lappeenranta, FinlandLappeenranta-Lahti University of TechnologyLappeenrantaFinlandLappeenranta-Lahti University of Technology, Lappeenranta, Finland†Deceased.M.BesanconF.CoudercM.DejardinD.DenegriJ.L.FaureF.FerriS.GanjourP.GrasG.Hamel de MonchenaultV.LohezicJ.MalclesJ.RanderA.RosowskyM.Ö.SahinA.Savoy-Navarro22P.SimkinaM.TitovM.TornagoIRFU, CEA, Université Paris-Saclay, Gif-sur-Yvette, FranceIRFUCEAUniversité Paris-SaclayGif-sur-YvetteFranceIRFU, CEA, Université Paris-Saclay, Gif-sur-Yvette, France22Also at Purdue University, West Lafayette, Indiana, USA.C.Baldenegro BarreraF.BeaudetteA.Buchot PerraguinP.BussonA.CappatiC.CharlotF.DamasO.DavignonA.De WitG.FalmagneB.A.Fontana Santos AlvesS.GhoshA.GilbertR.Granier de CassagnacA.HakimiB.HarikrishnanL.KalipolitiG.LiuJ.MottaM.NguyenC.OchandoL.PortalesR.SalernoJ.B.SauvanY.SiroisA.TarabiniE.VernazzaA.ZabiA.ZghicheLaboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, FranceLaboratoire Leprince-RinguetCNRS/IN2P3Ecole PolytechniqueInstitut Polytechnique de ParisPalaiseauFranceLaboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, FranceJ.-L.Agram23J.AndreaD.ApparuD.BlochJ.-M.BromE.C.ChabertC.CollardS.FalkeU.GoerlachC.GrimaultR.HaeberleA.-C.Le BihanM.MeenaG.SahaM.A.SessiniP.Van HoveUniversité de Strasbourg, CNRS, IPHC UMR 7178, Strasbourg, FranceUniversité de StrasbourgCNRSIPHC UMR 7178StrasbourgFranceUniversité de Strasbourg, CNRS, IPHC UMR 7178, Strasbourg, France23Also at Université de Haute Alsace, Mulhouse, France.S.BeauceronB.BlanconG.BoudoulN.ChanonJ.ChoiD.ContardoP.DepasseC.Dozen24H.El MamouniJ.FayS.GasconM.GouzevitchC.GreenbergG.GrenierB.IlleI.B.LaktinehM.LethuillierL.MirabitoS.PerriesA.PurohitM.Vander DoncktP.VerdierJ.XiaoInstitut de Physique des 2 Infinis de Lyon (IP2I), Villeurbanne, FranceInstitut de Physique des 2 Infinis de Lyon (IP2I)VilleurbanneFranceInstitut de Physique des 2 Infinis de Lyon (IP2I ), Villeurbanne, France24Also at Department of Physics, Tsinghua University, Beijing, China.A.Khvedelidze17I.LomidzeZ.Tsamalaidze17Georgian Technical University, Tbilisi, GeorgiaGeorgian Technical UniversityTbilisiGeorgiaGeorgian Technical University, Tbilisi, GeorgiaV.BottaL.FeldK.KleinM.LipinskiD.MeuserA.PaulsN.RöwertM.TeroerdeRWTH Aachen University, I. Physikalisches Institut, Aachen, GermanyRWTH Aachen UniversityI. Physikalisches InstitutAachenGermanyRWTH Aachen University, I. Physikalisches Institut, Aachen, GermanyS.DiekmannA.DodonovaN.EichD.EliseevF.EngelkeM.ErdmannP.FackeldeyB.FischerT.HebbekerK.HoepfnerF.IvoneA.JungM.y.LeeL.MastrolorenzoF.MausolfM.MerschmeyerA.MeyerS.MukherjeeD.NollA.NovakF.NowotnyA.PozdnyakovY.RathW.RedjebF.RehmH.ReithlerU.SarkarV.SarkisoviA.SchmidtA.SharmaJ.L.SpahA.SteinF.Torres Da Silva De Araujo25L.VigilanteS.WiedenbeckS.ZaleskiRWTH Aachen University, III. Physikalisches Institut A, Aachen, GermanyRWTH Aachen UniversityIII. Physikalisches Institut AAachenGermanyRWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany25Also at The University of the State of Amazonas, Manaus, Brazil.C.DziwokG.FlüggeW.Haj Ahmad26T.KressA.NowackO.PoothA.StahlT.ZiemonsA.ZotzRWTH Aachen University, III. Physikalisches Institut B, Aachen, GermanyRWTH Aachen UniversityIII. Physikalisches Institut BAachenGermanyRWTH Aachen University, III. Physikalisches Institut B, Aachen, Germany26Also at Erzincan Binali Yildirim University, Erzincan, Turkey.H.Aarup PetersenM.Aldaya MartinJ.AlimenaS.AmorosoY.AnS.BaxterM.BayatmakouH.Becerril GonzalezO.BehnkeA.BelvedereS.BhattacharyaF.Blekman27K.Borras28D.BrunnerA.CampbellA.CardiniC.ChengF.ColombinaS.Consuegra RodríguezG.Correia SilvaM.De SilvaG.EckerlinD.EcksteinL.I.Estevez BanosO.FilatovE.Gallo27A.GeiserA.GiraldiG.GreauV.GuglielmiM.GuthoffA.HinzmannA.Jafari29L.JeppeN.Z.JomhariB.KaechM.KasemannH.KavehC.KleinwortR.KoglerM.KommD.KrückerW.LangeD.Leyva PerniaK.Lipka30W.Lohmann31R.MankelI.-A.Melzer-PellmannM.Mendizabal MorentinJ.MetwallyA.B.MeyerG.MilellaA.MussgillerL.P.NairA.NürnbergY.OtaridJ.ParkD.Pérez AdánE.RankenA.RasperezaB.Ribeiro LopesJ.RübenachA.SaggioM.Scham3228S.Schnake28P.SchützeC.Schwanenberger27D.SelivanovaM.ShchedrolosievR.E.Sosa RicardoD.StaffordF.VazzolerA.Ventura BarrosoR.WalshQ.WangY.WenK.WichmannL.Wiens28C.WissingY.YangA.Zimermmane Castro SantosDeutsches Elektronen-Synchrotron, Hamburg, GermanyDeutsches Elektronen-SynchrotronHamburgGermanyDeutsches Elektronen-Synchrotron, Hamburg, Germany27Also at University of Hamburg, Hamburg, Germany.28Also at RWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany.29Also at Isfahan University of Technology, Isfahan, Iran.30Also at Bergische University Wuppertal (BUW), Wuppertal, Germany.31Also at Brandenburg University of Technology, Cottbus, Germany.32Also at Forschungszentrum Jülich, Juelich, Germany.A.AlbrechtS.AlbrechtM.AntonelloS.BeinL.BenatoM.BonanomiP.ConnorM.EichK.El MorabitY.FischerA.FröhlichC.GarbersE.GaruttiA.GrohsjeanM.HajheidariJ.HallerH.R.JabuschG.KasieczkaP.KeicherR.KlannerW.KorcariT.KramerV.KutznerF.LabeJ.LangeA.LobanovC.MatthiesA.MehtaL.MoureauxM.MrowietzA.NigamovaY.NissanA.PaaschK.J.Pena RodriguezT.QuadfaselB.RacitiM.RiegerD.SavoiuJ.SchindlerP.SchleperM.SchröderJ.SchwandtM.SommerhalderH.StadieG.SteinbrückA.TewsM.WolfUniversity of Hamburg, Hamburg, GermanyUniversity of HamburgHamburgGermanyUniversity of Hamburg, Hamburg, GermanyS.BrommerM.BurkartE.ButzT.ChwalekA.DierlammA.DrollN.FaltermannM.GiffelsA.GottmannF.Hartmann33R.HofsaessM.HorzelaU.HusemannJ.KieselerM.KluteR.KoppenhöferJ.M.LawhornM.LinkA.LintuluotoS.MaierS.MitraM.MormileTh.MüllerM.NeukumM.OhM.PresillaG.QuastK.RabbertzB.RegneryN.ShadskiyI.ShvetsovH.J.SimonisM.Toms34N.TrevisaniR.UlrichR.F.Von CubeM.WassmerS.WielandF.WittigR.WolfS.WunschX.ZuoKarlsruher Institut fuer Technologie, Karlsruhe, GermanyKarlsruher Institut fuer TechnologieKarlsruheGermanyKarlsruher Institut fuer Technologie, Karlsruhe, Germany33Also at CERN, European Organization for Nuclear Research, Geneva, Switzerland.34Now at an institute or an international laboratory covered by a cooperation agreement with CERN.G.AnagnostouG.DaskalakisA.KyriakisA.Papadopoulos33A.StakiaInstitute of Nuclear and Particle Physics (INPP), NCSR Demokritos, Aghia Paraskevi, GreeceInstitute of Nuclear and Particle Physics (INPP)NCSR DemokritosAghia ParaskeviGreeceInstitute of Nuclear and Particle Physics (INPP), NCSR Demokritos, Aghia Paraskevi, GreeceP.KontaxakisG.MelachroinosA.PanagiotouI.PapavergouI.ParaskevasN.SaoulidouK.TheofilatosE.TziaferiK.VellidisI.ZisopoulosNational and Kapodistrian University of Athens, Athens, GreeceNational and Kapodistrian University of AthensAthensGreeceNational and Kapodistrian University of Athens, Athens, GreeceG.BakasT.ChatzistavrouG.KarapostoliK.KousourisI.PapakrivopoulosE.SiamarkouG.TsipolitisA.ZacharopoulouNational Technical University of Athens, Athens, GreeceNational Technical University of AthensAthensGreeceNational Technical University of Athens, Athens, GreeceK.AdamidisI.BestintzanosI.EvangelouC.FoudasP.GianneiosC.KamtsikisP.KatsoulisP.KokkasP.G.Kosmoglou KioseoglouN.ManthosI.PapadopoulosJ.StrologasUniversity of Ioánnina, Ioánnina, GreeceUniversity of IoánninaIoánninaGreeceUniversity of Ioánnina, Ioánnina, GreeceM.Bartók35C.HajduD.Horvath3637F.SiklerV.VeszpremiHUN-REN Wigner Research Centre for Physics, Budapest, HungaryHUN-REN Wigner Research Centre for PhysicsBudapestHungaryHUN-REN Wigner Research Centre for Physics, Budapest, Hungary35Also at Institute of Physics, University of Debrecen, Debrecen, Hungary.36Also at Institute of Nuclear Research ATOMKI, Debrecen, Hungary.37Now at Universitatea Babes-Bolyai - Facultatea de Fizica, Cluj-Napoca, Romania.M.CsanádK.FarkasM.M.A.Gadallah38Á.KadlecsikP.MajorK.MandalG.PásztorA.J.Rádl39G.I.VeresMTA-ELTE Lendület CMS Particle and Nuclear Physics Group, Eötvös Loránd University, Budapest, HungaryMTA-ELTE Lendület CMS Particle and Nuclear Physics GroupEötvös Loránd UniversityBudapestHungaryMTA-ELTE Lendület CMS Particle and Nuclear Physics Group, Eötvös Loránd University, Budapest, Hungary38Also at Physics Department, Faculty of Science, Assiut University, Assiut, Egypt.39Also at HUN-REN Wigner Research Centre for Physics, Budapest, Hungary.P.RaicsB.UjvariG.ZiliziFaculty of Informatics, University of Debrecen, Debrecen, HungaryFaculty of InformaticsUniversity of DebrecenDebrecenHungaryFaculty of Informatics, University of Debrecen, Debrecen, HungaryG.BenczeS.CzellarJ.Karancsi35J.MolnarZ.SzillasiInstitute of Nuclear Research ATOMKI, Debrecen, HungaryInstitute of Nuclear Research ATOMKIDebrecenHungaryInstitute of Nuclear Research ATOMKI, Debrecen, HungaryT.Csorgo39F.Nemes39T.NovakKaroly Robert Campus, MATE Institute of Technology, Gyongyos, HungaryMATE Institute of TechnologyKaroly Robert CampusGyongyosHungaryKaroly Robert Campus, MATE Institute of Technology, Gyongyos, HungaryJ.BabbarS.BansalS.B.BeriV.BhatnagarG.ChaudharyS.ChauhanN.Dhingra40A.KaurA.KaurH.KaurM.KaurS.KumarK.SandeepT.SheokandJ.B.SinghA.SinglaPanjab University, Chandigarh, IndiaPanjab UniversityChandigarhIndiaPanjab University, Chandigarh, India40Also at Punjab Agricultural University, Ludhiana, India.A.AhmedA.BhardwajA.ChhetriB.C.ChoudharyA.KumarA.KumarM.NaimuddinK.RanjanS.SaumyaUniversity of Delhi, Delhi, IndiaUniversity of DelhiDelhiIndiaUniversity of Delhi, Delhi, IndiaS.BaradiaS.Barman41S.BhattacharyaS.DuttaS.DuttaP.PalitS.SarkarSaha Institute of Nuclear Physics, HBNI, Kolkata, IndiaSaha Institute of Nuclear PhysicsHBNIKolkataIndiaSaha Institute of Nuclear Physics, HBNI, Kolkata, India41Also at University of Visva-Bharati, Santiniketan, India.M.M.AmeenP.K.BeheraS.C.BeheraS.ChatterjeeP.JanaP.KalbhorJ.R.Komaragiri42D.Kumar42L.Panwar42P.R.PujahariN.R.SahaA.SharmaA.K.SikdarS.VermaIndian Institute of Technology Madras, Madras, IndiaIndian Institute of Technology MadrasMadrasIndiaIndian Institute of Technology Madras, Madras, India42Also at Indian Institute of Science (IISc), Bangalore, India.S.DugadM.KumarG.B.MohantyP.SuryadevaraTata Institute of Fundamental Research-A, Mumbai, IndiaTata Institute of Fundamental Research-AMumbaiIndiaTata Institute of Fundamental Research-A, Mumbai, IndiaA.BalaS.BanerjeeR.M.ChatterjeeM.GuchaitSh.JainS.KarmakarS.KumarG.MajumderK.MazumdarS.ParoliaA.ThachayathTata Institute of Fundamental Research-B, Mumbai, IndiaTata Institute of Fundamental Research-BMumbaiIndiaTata Institute of Fundamental Research-B, Mumbai, IndiaS.Bahinipati43A.K.DasC.KarD.Maity44P.MalT.MishraV.K.Muraleedharan Nair Bindhu44K.Naskar44A.Nayak44P.SadangiP.SahaS.K.SwainS.Varghese44D.Vats44National Institute of Science Education and Research, An OCC of Homi Bhabha National Institute, Bhubaneswar, Odisha, IndiaNational Institute of Science Education and ResearchAn OCC of Homi Bhabha National InstituteBhubaneswarOdishaIndiaNational Institute of Science Education and Research, An OCC of Homi Bhabha National Institute, Bhubaneswar, Odisha, India43Also at IIT Bhubaneswar, Bhubaneswar, India.44Also at Institute of Physics, Bhubaneswar, India.S.Acharya45A.AlpanaS.DubeB.Gomber45B.KansalA.LahaB.Sahu45S.SharmaIndian Institute of Science Education and Research (IISER), Pune, IndiaIndian Institute of Science Education and Research (IISER)PuneIndiaIndian Institute of Science Education and Research (IISER), Pune, India45Also at University of Hyderabad, Hyderabad, India.H.Bakhshiansohi46E.Khazaie47M.Zeinali48Isfahan University of Technology, Isfahan, IranIsfahan University of TechnologyIsfahanIranIsfahan University of Technology, Isfahan, Iran46Also at Deutsches Elektronen-Synchrotron, Hamburg, Germany.47Also at Department of Physics, Isfahan University of Technology, Isfahan, Iran.48Also at Sharif University of Technology, Tehran, Iran.S.Chenarani49S.M.EtesamiM.KhakzadM.Mohammadi NajafabadiInstitute for Research in Fundamental Sciences (IPM), Tehran, IranInstitute for Research in Fundamental Sciences (IPM)TehranIranInstitute for Research in Fundamental Sciences (IPM), Tehran, Iran49Also at Department of Physics, University of Science and Technology of Mazandaran, Behshahr, Iran.M.GrunewaldUniversity College Dublin, Dublin, IrelandUniversity College DublinDublinIrelandUniversity College Dublin, Dublin, IrelandM.AbbresciaabR.Alyac50A.ColaleoabD.CreanzaacB.D'AnziabN.De FilippisacM.De PalmaabA.Di FlorioacW.Elmetenaweeab50L.FioreaG.IaselliacM.LoukaabG.MaggiacM.MaggiaI.MargjekaabV.MastrapasquaabS.MyabS.NuzzoabA.PellecchiaabA.PompiliabG.PuglieseacR.RadognaaG.Ramirez-SanchezacD.RamosaA.RanieriaL.SilvestrisaF.M.SimoneabÜ.SözbiliraA.StamerraaR.VendittiaP.VerwilligenaA.ZazaabaINFN Sezione di Bari, Bari, ItalyINFN Sezione di BariBariItalyINFN Sezione di Bari, Bari, ItalybUniversità di Bari, Bari, ItalyUniversità di BariBariItalyUniversità di Bari, Bari, ItalycPolitecnico di Bari, Bari, ItalyPolitecnico di BariBariItalyPolitecnico di Bari, Bari, Italy50Also at Helwan University, Cairo, Egypt.G.AbbiendiaC.BattilanaabD.BonacorsiabL.BorgonoviaR.CampaniniabP.CapiluppiabA.CastroabF.R.CavalloaM.CuffianiabG.M.DallavalleaT.DiotaleviabF.FabbriaA.FanfaniabD.FasanellaabP.GiacomelliaL.GiommiabC.GrandiaL.GuiducciabS.Lo Meoa51L.LunertiabS.MarcelliniaG.MasettiaF.L.NavarriaabA.PerrottaaF.PrimaveraabA.M.RossiabG.P.SiroliabaINFN Sezione di Bologna, Bologna, ItalyINFN Sezione di BolognaBolognaItalyINFN Sezione di Bologna, Bologna, ItalybUniversità di Bologna, Bologna, ItalyUniversità di BolognaBolognaItalyUniversità di Bologna, Bologna, Italy51Also at Italian National Agency for New Technologies, Energy and Sustainable Economic Development, Bologna, Italy.S.Costaab52A.Di MattiaaR.PotenzaabA.Tricomiab52C.TuveabaINFN Sezione di Catania, Catania, ItalyINFN Sezione di CataniaCataniaItalyINFN Sezione di Catania, Catania, ItalybUniversità di Catania, Catania, ItalyUniversità di CataniaCataniaItalyUniversità di Catania, Catania, Italy52Also at Centro Siciliano di Fisica Nucleare e di Struttura Della Materia, Catania, Italy.P.AssiourasaG.BarbagliaG.BardelliabB.CamaianiabA.CasseseaR.CeccarelliaV.CiulliabC.CivininiaR.D'AlessandroabE.FocardiabT.KelloaG.LatinoabP.LenziabM.LizzoaM.MeschiniaS.PaolettiaA.PapanastassiouabG.SguazzoniaL.VilianiaaINFN Sezione di Firenze, Firenze, ItalyINFN Sezione di FirenzeFirenzeItalyINFN Sezione di Firenze, Firenze, ItalybUniversità di Firenze, Firenze, ItalyUniversità di FirenzeFirenzeItalyUniversità di Firenze, Firenze, ItalyL.BenussiS.BiancoS.Meola53D.PiccoloINFN Laboratori Nazionali di Frascati, Frascati, ItalyINFN Laboratori Nazionali di FrascatiFrascatiItalyINFN Laboratori Nazionali di Frascati, Frascati, Italy53Also at Università degli Studi Guglielmo Marconi, Roma, Italy.P.ChatagnonaF.FerroaE.RobuttiaS.TosiabaINFN Sezione di Genova, Genova, ItalyINFN Sezione di GenovaGenovaItalyINFN Sezione di Genova, Genova, ItalybUniversità di Genova, Genova, ItalyUniversità di GenovaGenovaItalyUniversità di Genova, Genova, ItalyA.BenagliaaG.BoldriniabF.BrivioaF.CetorelliaF.De GuioabM.E.DinardoabP.DiniaS.GennaiaR.GerosaabA.GhezziabP.GovoniabL.GuzziaM.T.LucchiniabM.MalbertiaS.MalvezziaA.MassironiaD.MenasceaL.MoroniaM.PaganoniabD.PedriniaB.S.PinoliniaS.RagazziabT.Tabarelli de FatisabD.ZuoloaaINFN Sezione di Milano-Bicocca, Milano, ItalyINFN Sezione di Milano-BicoccaMilanoItalyINFN Sezione di Milano-Bicocca, Milano, ItalybUniversità di Milano-Bicocca, Milano, ItalyUniversità di Milano-BicoccaMilanoItalyUniversità di Milano-Bicocca, Milano, ItalyS.BuontempoaA.CagnottaabF.CarnevaliabN.CavalloacA.De IorioabF.FabozziacA.O.M.IorioabL.Listaab54P.Paoluccia33B.RossiaC.SciaccaabaINFN Sezione di Napoli, Napoli, ItalyINFN Sezione di NapoliNapoliItalyINFN Sezione di Napoli, Napoli, ItalybUniversità di Napoli ‘Federico II’, Napoli, ItalyUniversità di Napoli ‘Federico II’NapoliItalyUniversità di Napoli ‘Federico II’, Napoli, ItalycUniversità della Basilicata, Potenza, ItalyUniversità della BasilicataPotenzaItalyUniversità della Basilicata, Potenza, ItalydUniversità G. Marconi, Roma, ItalyUniversità G. MarconiRomaItalyUniversità G. Marconi, Roma, Italy54Also at Scuola Superiore Meridionale, Università di Napoli ‘Federico II’, Napoli, Italy.R.ArdinoaP.AzziaN.Bacchettaa55D.BiselloabP.BortignonaA.BragagnoloabR.CarlinabP.ChecchiaaT.DorigoaF.FanzagoaU.GaspariniabF.GonellaaE.LusianiaM.MargoniabM.MiglioriniabJ.PazziniabP.RoncheseabR.RossinabF.SimonettoabG.StrongaM.TosiabA.TriossiabS.VenturaaH.YararabM.ZanettiabP.ZottoabA.ZucchettaabG.ZumerleabaINFN Sezione di Padova, Padova, ItalyINFN Sezione di PadovaPadovaItalyINFN Sezione di Padova, Padova, ItalybUniversità di Padova, Padova, ItalyUniversità di PadovaPadovaItalyUniversità di Padova, Padova, ItalycUniversità di Trento, Trento, ItalyUniversità di TrentoTrentoItalyUniversità di Trento, Trento, Italy55Also at Fermi National Accelerator Laboratory, Batavia, Illinois, USA.S.Abu Zeida56C.AimèabA.BraghieriaS.CalzaferriaD.FiorinaaP.MontagnaabV.ReaC.RiccardiabP.SalviniaI.VaiabP.VituloabaINFN Sezione di Pavia, Pavia, ItalyINFN Sezione di PaviaPaviaItalyINFN Sezione di Pavia, Pavia, ItalybUniversità di Pavia, Pavia, ItalyUniversità di PaviaPaviaItalyUniversità di Pavia, Pavia, Italy56Also at Ain Shams University, Cairo, Egypt.S.AjmalabP.Asenova57G.M.BileiaD.CiangottiniabL.FanòabM.MagheriniabG.MantovaniabV.MarianiabM.MenichelliaF.Moscatellia57A.RossiabA.SantocchiaabD.SpigaaT.TedeschiabaINFN Sezione di Perugia, Perugia, ItalyINFN Sezione di PerugiaPerugiaItalyINFN Sezione di Perugia, Perugia, ItalybUniversità di Perugia, Perugia, ItalyUniversità di PerugiaPerugiaItalyUniversità di Perugia, Perugia, Italy57Also at Consiglio Nazionale delle Ricerche - Istituto Officina dei Materiali, Perugia, Italy.P.AzzurriaG.BagliesiaR.BhattacharyaaL.BianchiniabT.BoccaliaE.BossiniaD.BruschiniacR.CastaldiaM.A.CiocciabM.CiprianiabV.D'AmanteadR.Dell'OrsoaS.DonatoaA.GiassiaF.LigabueacD.Matos FigueiredoaA.MessineoabM.MusichabF.PallaaA.RizziabG.RolandiacS.Roy ChowdhuryaT.SarkaraA.ScribanoaP.SpagnoloaR.TenchiniaG.TonelliabN.TuriniadA.VenturiaP.G.VerdiniaaINFN Sezione di Pisa, Pisa, ItalyINFN Sezione di PisaPisaItalyINFN Sezione di Pisa, Pisa, ItalybUniversità di Pisa, Pisa, ItalyUniversità di PisaPisaItalyUniversità di Pisa, Pisa, ItalycScuola Normale Superiore di Pisa, Pisa, ItalyScuola Normale Superiore di PisaPisaItalyScuola Normale Superiore di Pisa, Pisa, ItalydUniversità di Siena, Siena, ItalyUniversità di SienaSienaItalyUniversità di Siena, Siena, ItalyP.BarriaaM.CampanaabF.CavallariaL.Cunqueiro MendezabD.Del ReabE.Di MarcoaM.DiemozaF.ErricoabE.LongoabP.MeridianiaJ.MijuskovicabG.OrgantiniabF.PandolfiaR.ParamattiabC.QuarantaabS.RahatlouabC.RovelliaF.SantanastasioabL.SoffiaaINFN Sezione di Roma, Roma, ItalyINFN Sezione di RomaRomaItalyINFN Sezione di Roma, Roma, ItalybSapienza Università di Roma, Roma, ItalySapienza Università di RomaRomaItalySapienza Università di Roma, Roma, ItalyN.AmapaneabR.ArcidiaconoacS.ArgiroabM.ArneodoacN.BartosikaR.BellanabA.BelloraabC.BiinoaN.CartigliaaM.CostaabR.CovarelliabN.DemariaaL.FincoaM.GrippoabB.KianiabF.LeggeraF.LuongoabC.MariottiaS.MaselliaA.MeccaabE.MiglioreabM.MontenoaR.MulargiaaM.M.ObertinoabG.OrtonaaL.PacherabN.PastroneaM.PelliccioniaM.RuspaacF.SivieroabV.SolaabA.SolanoabA.StaianoaC.TarriconeabD.TrocinoaG.UmoretabE.VlasovabaINFN Sezione di Torino, Torino, ItalyINFN Sezione di TorinoTorinoItalyINFN Sezione di Torino, Torino, ItalybUniversità di Torino, Torino, ItalyUniversità di TorinoTorinoItalyUniversità di Torino, Torino, ItalycUniversità del Piemonte Orientale, Novara, ItalyUniversità del Piemonte OrientaleNovaraItalyUniversità del Piemonte Orientale, Novara, ItalyS.BelforteaV.CandeliseabM.CasarsaaF.CossuttiaK.De LeoabG.Della RiccaabaINFN Sezione di Trieste, Trieste, ItalyINFN Sezione di TriesteTriesteItalyINFN Sezione di Trieste, Trieste, ItalybUniversità di Trieste, Trieste, ItalyUniversità di TriesteTriesteItalyUniversità di Trieste, Trieste, ItalyS.DograJ.HongC.HuhB.KimD.H.KimJ.KimH.LeeS.W.LeeC.S.MoonY.D.OhM.S.RyuS.SekmenY.C.YangKyungpook National University, Daegu, KoreaKyungpook National UniversityDaeguKoreaKyungpook National University, Daegu, KoreaM.S.KimDepartment of Mathematics and Physics - GWNU, Gangneung, KoreaDepartment of Mathematics and Physics - GWNUGangneungKoreaDepartment of Mathematics and Physics - GWNU, Gangneung, KoreaG.BakP.GwakH.KimD.H.MoonChonnam National University, Institute for Universe and Elementary Particles, Kwangju, KoreaChonnam National UniversityInstitute for Universe and Elementary ParticlesKwangjuKoreaChonnam National University, Institute for Universe and Elementary Particles, Kwangju, KoreaE.AsilarD.KimT.J.KimJ.A.MerlinHanyang University, Seoul, KoreaHanyang UniversitySeoulKoreaHanyang University, Seoul, KoreaS.ChoiS.HanB.HongK.LeeK.S.LeeS.LeeJ.ParkS.K.ParkJ.YooKorea University, Seoul, KoreaKorea UniversitySeoulKoreaKorea University, Seoul, KoreaJ.GohS.YangKyung Hee University, Department of Physics, Seoul, KoreaKyung Hee UniversityDepartment of PhysicsSeoulKoreaKyung Hee University, Department of Physics, Seoul, KoreaH.S.KimY.KimS.LeeSejong University, Seoul, KoreaSejong UniversitySeoulKoreaSejong University, Seoul, KoreaJ.AlmondJ.H.BhyunJ.ChoiW.JunJ.KimJ.S.KimS.KoH.KwonH.LeeJ.LeeJ.LeeB.H.OhS.B.OhH.SeoU.K.YangI.YoonSeoul National University, Seoul, KoreaSeoul National UniversitySeoulKoreaSeoul National University, Seoul, KoreaW.JangD.Y.KangY.KangS.KimB.KoJ.S.H.LeeY.LeeI.C.ParkY.RohI.J.WatsonUniversity of Seoul, Seoul, KoreaUniversity of SeoulSeoulKoreaUniversity of Seoul, Seoul, KoreaS.HaH.D.YooYonsei University, Department of Physics, Seoul, KoreaYonsei UniversityDepartment of PhysicsSeoulKoreaYonsei University, Department of Physics, Seoul, KoreaM.ChoiM.R.KimH.LeeY.LeeI.YuSungkyunkwan University, Suwon, KoreaSungkyunkwan UniversitySuwonKoreaSungkyunkwan University, Suwon, KoreaT.BeyrouthyY.MaghrbiCollege of Engineering and Technology, American University of the Middle East (AUM), Dasman, KuwaitCollege of Engineering and TechnologyAmerican University of the Middle East (AUM)DasmanKuwaitCollege of Engineering and Technology, American University of the Middle East (AUM), Dasman, KuwaitK.DreimanisA.GaileG.PikursA.PotrebkoM.SeidelV.Veckalns58Riga Technical University, Riga, LatviaRiga Technical UniversityRigaLatviaRiga Technical University, Riga, Latvia58Also at Riga Technical University, Riga, Latvia.N.R.StrautnieksUniversity of Latvia (LU), Riga, LatviaUniversity of Latvia (LU)RigaLatviaUniversity of Latvia (LU), Riga, LatviaM.AmbrozasA.JuodagalvisA.RinkeviciusG.TamulaitisVilnius University, Vilnius, LithuaniaVilnius UniversityVilniusLithuaniaVilnius University, Vilnius, LithuaniaN.Bin NorjoharuddeenI.Yusuff59Z.ZolkapliNational Centre for Particle Physics, Universiti Malaya, Kuala Lumpur, MalaysiaNational Centre for Particle PhysicsUniversiti MalayaKuala LumpurMalaysiaNational Centre for Particle Physics, Universiti Malaya, Kuala Lumpur, Malaysia59Also at Department of Applied Physics, Faculty of Science and Technology, Universiti Kebangsaan Malaysia, Bangi, Malaysia.J.F.BenitezA.Castaneda HernandezH.A.Encinas AcostaL.G.Gallegos MaríñezM.León CoelloJ.A.Murillo QuijadaA.SehrawatL.Valencia PalomoUniversidad de Sonora (UNISON), Hermosillo, MexicoUniversidad de Sonora (UNISON)HermosilloMexicoUniversidad de Sonora (UNISON), Hermosillo, MexicoG.AyalaH.Castilla-ValdezE.De La Cruz-BureloI.Heredia-De La Cruz60R.Lopez-FernandezC.A.Mondragon HerreraA.Sánchez HernándezCentro de Investigacion y de Estudios Avanzados del IPN, Mexico City, MexicoCentro de Investigacion y de Estudios Avanzados del IPNMexico CityMexicoCentro de Investigacion y de Estudios Avanzados del IPN, Mexico City, Mexico60Also at Consejo Nacional de Ciencia y Tecnología, Mexico City, Mexico.C.Oropeza BarreraM.Ramírez GarcíaUniversidad Iberoamericana, Mexico City, MexicoUniversidad IberoamericanaMexico CityMexicoUniversidad Iberoamericana, Mexico City, MexicoI.BautistaI.PedrazaH.A.Salazar IbarguenC.Uribe EstradaBenemerita Universidad Autonoma de Puebla, Puebla, MexicoBenemerita Universidad Autonoma de PueblaPueblaMexicoBenemerita Universidad Autonoma de Puebla, Puebla, MexicoI.BubanjaN.RaicevicUniversity of Montenegro, Podgorica, MontenegroUniversity of MontenegroPodgoricaMontenegroUniversity of Montenegro, Podgorica, MontenegroP.H.ButlerUniversity of Canterbury, Christchurch, New ZealandUniversity of CanterburyChristchurchNew ZealandUniversity of Canterbury, Christchurch, New ZealandA.AhmadM.I.AsgharA.AwaisM.I.M.AwanH.R.HooraniW.A.KhanNational Centre for Physics, Quaid-I-Azam University, Islamabad, PakistanNational Centre for PhysicsQuaid-I-Azam UniversityIslamabadPakistanNational Centre for Physics, Quaid-I-Azam University, Islamabad, PakistanV.AvatiL.GrzankaM.MalawskiAGH University of Krakow, Faculty of Computer Science, Electronics and Telecommunications, Krakow, PolandAGH University of KrakowFaculty of Computer Science, Electronics and TelecommunicationsKrakowPolandAGH University of Krakow, Faculty of Computer Science, Electronics and Telecommunications, Krakow, PolandH.BialkowskaM.BlujB.BoimskaM.GórskiM.KazanaM.SzleperP.ZalewskiNational Centre for Nuclear Research, Swierk, PolandNational Centre for Nuclear ResearchSwierkPolandNational Centre for Nuclear Research, Swierk, PolandK.BunkowskiK.DorobaA.KalinowskiM.KoneckiJ.KrolikowskiA.MuhammadInstitute of Experimental Physics, Faculty of Physics, University of Warsaw, Warsaw, PolandInstitute of Experimental PhysicsFaculty of PhysicsUniversity of WarsawWarsawPolandInstitute of Experimental Physics, Faculty of Physics, University of Warsaw, Warsaw, PolandK.PozniakW.ZabolotnyWarsaw University of Technology, Warsaw, PolandWarsaw University of TechnologyWarsawPolandWarsaw University of Technology, Warsaw, PolandM.AraujoD.BastosC.Beirão Da Cruz E SilvaA.BolettiM.BozzoT.CamporesiG.Da MolinP.FaccioliM.GallinaroJ.HollarN.LeonardoT.NiknejadA.PetrilliM.PisanoJ.SeixasJ.VarelaJ.W.WulffLaboratório de Instrumentação e Física Experimental de Partículas, Lisboa, PortugalLaboratório de Instrumentação e Física Experimental de PartículasLisboaPortugalLaboratório de Instrumentação e Física Experimental de Partículas, Lisboa, PortugalP.AdzicP.MilenovicFaculty of Physics, University of Belgrade, Belgrade, SerbiaFaculty of PhysicsUniversity of BelgradeBelgradeSerbiaFaculty of Physics, University of Belgrade, Belgrade, SerbiaM.DordevicJ.MilosevicV.RekovicVINCA Institute of Nuclear Sciences, University of Belgrade, Belgrade, SerbiaVINCA Institute of Nuclear SciencesUniversity of BelgradeBelgradeSerbiaVINCA Institute of Nuclear Sciences, University of Belgrade, Belgrade, SerbiaM.Aguilar-BenitezJ.Alcaraz MaestreCristina F.BedoyaM.CepedaM.CerradaN.ColinoB.De La CruzA.Delgado PerisA.Escalante Del ValleD.Fernández Del ValJ.P.Fernández RamosJ.FlixM.C.FouzO.Gonzalez LopezS.Goy LopezJ.M.HernandezM.I.JosaD.MoranC.M.Morcillo PerezÁ.Navarro TobarC.Perez DengraA.Pérez-Calero YzquierdoJ.Puerta PelayoI.RedondoD.D.Redondo FerreroL.RomeroS.Sánchez NavasL.Urda GómezJ.Vazquez EscobarC.WillmottCentro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, SpainCentro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT)MadridSpainCentro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, SpainJ.F.de TrocónizUniversidad Autónoma de Madrid, Madrid, SpainUniversidad Autónoma de MadridMadridSpainUniversidad Autónoma de Madrid, Madrid, SpainB.Alvarez GonzalezJ.CuevasJ.Fernandez MenendezS.FolguerasI.Gonzalez CaballeroJ.R.González FernándezE.Palencia CortezonC.Ramón ÁlvarezV.Rodríguez BouzaA.Soto RodríguezA.TrapoteC.Vico VillalbaP.VischiaUniversidad de Oviedo, Instituto Universitario de Ciencias y Tecnologías Espaciales de Asturias (ICTEA), Oviedo, SpainUniversidad de OviedoInstituto Universitario de Ciencias y Tecnologías Espaciales de Asturias (ICTEA)OviedoSpainUniversidad de Oviedo, Instituto Universitario de Ciencias y Tecnologías Espaciales de Asturias (ICTEA), Oviedo, SpainS.BhowmikS.Blanco FernándezJ.A.Brochero CifuentesI.J.CabrilloA.CalderonJ.Duarte CampderrosM.FernandezG.GomezC.Lasaosa GarcíaC.Martinez RiveroP.Martinez Ruiz del ArbolF.MatorrasP.Matorras CuevasE.Navarrete RamosJ.Piedra GomezL.ScodellaroI.VilaJ.M.Vizan GarciaInstituto de Física de Cantabria (IFCA), CSIC-Universidad de Cantabria, Santander, SpainInstituto de Física de Cantabria (IFCA)CSIC-Universidad de CantabriaSantanderSpainInstituto de Física de Cantabria (IFCA), CSIC-Universidad de Cantabria, Santander, SpainM.K.JayanandaB.Kailasapathy61D.U.J.SonnadaraD.D.C.WickramarathnaUniversity of Colombo, Colombo, Sri LankaUniversity of ColomboColomboSri LankaUniversity of Colombo, Colombo, Sri Lanka61Also at Trincomalee Campus, Eastern University, Sri Lanka, Nilaveli, Sri Lanka.W.G.D.Dharmaratna62K.LiyanageN.PereraN.WickramageUniversity of Ruhuna, Department of Physics, Matara, Sri LankaUniversity of RuhunaDepartment of PhysicsMataraSri LankaUniversity of Ruhuna, Department of Physics, Matara, Sri Lanka62Also at Saegis Campus, Nugegoda, Sri Lanka.D.AbbaneoC.AmendolaE.AuffrayG.AuzingerJ.BaechlerD.BarneyA.Bermúdez MartínezM.BiancoB.BilinA.A.Bin AnuarA.BocciE.BrondolinC.CaillolG.CerminaraN.ChernyavskayaD.d'EnterriaA.DabrowskiA.DavidA.De RoeckM.M.DefranchisM.DeileM.DobsonF.Fallavollita63L.ForthommeG.FranzoniW.FunkS.GianiD.GigiK.GillF.GlegeL.GouskosM.HarankoJ.HegemanB.HuberV.InnocenteT.JamesP.JanotS.LaurilaP.LecoqE.LeutgebC.LourençoB.MaierL.MalgeriM.MannelliA.C.MariniM.MatthewmanF.MeijersS.MersiE.MeschiV.MilosevicF.MontiF.MoortgatM.MuldersI.NeutelingsS.OrfanelliF.PantaleoG.PetruccianiA.PfeifferM.PieriniD.PiparoH.QuD.RabadyG.Reales GutiérrezM.RovereH.SakulinS.ScarfiC.SchwickM.SelvaggiA.SharmaK.ShchelinaP.SilvaP.Sphicas64A.G.Stahl LeitonA.SteenS.SummersD.TreilleP.TropeaA.TsirouD.WalterJ.Wanczyk65J.WangS.WuchterlP.ZehetnerP.ZejdlW.D.ZeunerCERN, European Organization for Nuclear Research, Geneva, SwitzerlandCERNEuropean Organization for Nuclear ResearchGenevaSwitzerlandCERN, European Organization for Nuclear Research, Geneva, Switzerland63Also at INFN Sezione di Pavia, Università di Pavia, Pavia, Italy.64Also at National and Kapodistrian University of Athens, Athens, Greece.65Also at Ecole Polytechnique Fédérale Lausanne, Lausanne, Switzerland.T.Bevilacqua66L.Caminada66A.EbrahimiW.ErdmannR.HorisbergerQ.IngramH.C.KaestliD.KotlinskiC.LangeM.Missiroli66L.Noehte66T.RohePaul Scherrer Institut, Villigen, SwitzerlandPaul Scherrer InstitutVilligenSwitzerlandPaul Scherrer Institut, Villigen, Switzerland66Also at Universität Zürich, Zurich, Switzerland.T.K.AarrestadK.Androsov65M.BackhausA.CalandriC.CazzanigaK.DattaA.De CosaG.DissertoriM.DittmarM.DonegàF.EbleM.GalliK.GediaF.GlessgenC.GrabD.HitsW.LustermannA.-M.LyonR.A.ManzoniM.MarchegianiL.MarcheseC.Martin PerezA.Mascellani65F.Nessi-TedaldiF.PaussV.PerovicS.PigazziniM.ReichmannC.ReisselT.ReitenspiessB.RisticF.RitiD.RuiniD.A.Sanz BecerraR.SeiditaJ.Steggemann65D.ValsecchiR.WallnyETH Zurich - Institute for Particle Physics and Astrophysics (IPA), Zurich, SwitzerlandETH ZurichInstitute for Particle Physics and Astrophysics (IPA)ZurichSwitzerlandETH Zurich - Institute for Particle Physics and Astrophysics (IPA), Zurich, SwitzerlandC.Amsler67P.BärtschiC.BottaD.BrzhechkoM.F.CanelliK.CormierR.Del BurgoJ.K.HeikkiläM.HuwilerW.JinA.JofreheiB.KilminsterS.LeontsinisS.P.LiechtiA.MacchioloP.MeiringV.M.MikuniU.MolinattiA.ReimersP.RobmannS.Sanchez CruzK.SchweigerM.SengerY.TakahashiR.TramontanoUniversität Zürich, Zurich, SwitzerlandUniversität ZürichZurichSwitzerlandUniversität Zürich, Zurich, Switzerland67Also at Stefan Meyer Institute for Subatomic Physics, Vienna, Austria.C.Adloff68D.BhowmikC.M.KuoW.LinP.K.RoutP.C.Tiwari42S.S.YuNational Central University, Chung-Li, TaiwanNational Central UniversityChung-LiTaiwanNational Central University, Chung-Li, Taiwan68Also at Laboratoire d'Annecy-le-Vieux de Physique des Particules, IN2P3-CNRS, Annecy-le-Vieux, France.L.CeardY.ChaoK.F.ChenP.s.ChenZ.g.ChenW.-S.HouT.h.HsuY.w.KaoR.KhuranaG.KoleY.y.LiR.-S.LuE.PaganisX.f.SuJ.Thomas-WilskerL.s.TsaiH.y.WuE.YazganNational Taiwan University (NTU), Taipei, TaiwanNational Taiwan University (NTU)TaipeiTaiwanNational Taiwan University (NTU), Taipei, TaiwanC.AsawatangtrakuldeeN.SrimanobhasV.WachirapusitanandHigh Energy Physics Research Unit, Department of Physics, Faculty of Science, Chulalongkorn University, Bangkok, ThailandHigh Energy Physics Research UnitDepartment of PhysicsFaculty of ScienceChulalongkorn UniversityBangkokThailandHigh Energy Physics Research Unit, Department of Physics, Faculty of Science, Chulalongkorn University, Bangkok, ThailandD.AgyelF.BoranZ.S.DemirogluF.DolekI.Dumanoglu69E.EskutY.Guler70E.Gurpinar Guler70C.IsikO.KaraA.Kayis TopaksuU.KiminsuG.OnengutK.Ozdemir71A.PolatozB.Tali72U.G.TokS.TurkcaparE.UslanI.S.ZorbakirÇukurova University, Physics Department, Science and Art Faculty, Adana, TurkeyÇukurova UniversityPhysics DepartmentScience and Art FacultyAdanaTurkeyÇukurova University, Physics Department, Science and Art Faculty, Adana, Turkey69Also at Near East University, Research Center of Experimental Health Science, Mersin, Turkey.70Also at Konya Technical University, Konya, Turkey.71Also at Izmir Bakircay University, Izmir, Turkey.72Also at Adiyaman University, Adiyaman, Turkey.M.Yalvac73Middle East Technical University, Physics Department, Ankara, TurkeyMiddle East Technical UniversityPhysics DepartmentAnkaraTurkeyMiddle East Technical University, Physics Department, Ankara, Turkey73Also at Bozok Universitetesi Rektörlügü, Yozgat, Turkey.B.AkgunI.O.AtakisiE.GülmezM.Kaya74O.Kaya75S.Tekten76Bogazici University, Istanbul, TurkeyBogazici UniversityIstanbulTurkeyBogazici University, Istanbul, Turkey74Also at Marmara University, Istanbul, Turkey.75Also at Milli Savunma University, Istanbul, Turkey.76Also at Kafkas University, Kars, Turkey.A.CakirK.Cankocak6977Y.KomurcuS.Sen78Istanbul Technical University, Istanbul, TurkeyIstanbul Technical UniversityIstanbulTurkeyIstanbul Technical University, Istanbul, Turkey77Now at stanbul Okan University, Istanbul, Turkey.78Also at Hacettepe University, Ankara, Turkey.O.AydilekS.Cerci72V.EpshteynB.HacisahinogluI.Hos79B.KaynakS.OzkorucukluO.PotokH.SertC.SimsekD.Sunar Cerci72C.ZorbilmezIstanbul University, Istanbul, TurkeyIstanbul UniversityIstanbulTurkeyIstanbul University, Istanbul, Turkey79Also at Istanbul University - Cerrahpasa, Faculty of Engineering, Istanbul, Turkey.B.Isildak80Yildiz Technical University, Istanbul, TurkeyYildiz Technical UniversityIstanbulTurkeyYildiz Technical University, Istanbul, Turkey80Also at Yildiz Technical University, Istanbul, Turkey.A.BoyaryntsevB.GrynyovInstitute for Scintillation Materials of National Academy of Science of Ukraine, Kharkiv, UkraineInstitute for Scintillation Materials of National Academy of Science of UkraineKharkivUkraineInstitute for Scintillation Materials of National Academy of Science of Ukraine, Kharkiv, UkraineL.LevchukNational Science Centre, Kharkiv Institute of Physics and Technology, Kharkiv, UkraineNational Science CentreKharkiv Institute of Physics and TechnologyKharkivUkraineNational Science Centre, Kharkiv Institute of Physics and Technology, Kharkiv, UkraineD.AnthonyJ.J.BrookeA.BundockF.BuryE.ClementD.CussansH.FlacherM.GlowackiJ.GoldsteinH.F.HeathL.KreczkoS.ParamesvaranS.Seif El Nasr-StoreyV.J.SmithN.Stylianou81K.Walkingshaw PassR.WhiteUniversity of Bristol, Bristol, United KingdomUniversity of BristolBristolUnited KingdomUniversity of Bristol, Bristol, United Kingdom81Also at Vrije Universiteit Brussel, Brussel, Belgium.A.H.BallK.W.BellA.Belyaev82C.BrewR.M.BrownD.J.A.CockerillC.CookeK.V.EllisK.HarderS.HarperM.-L.Holmberg83J.LinacreK.ManolopoulosD.M.NewboldE.OlaiyaD.PetytT.ReisG.SalviT.SchuhC.H.Shepherd-ThemistocleousI.R.TomalinT.WilliamsRutherford Appleton Laboratory, Didcot, United KingdomRutherford Appleton LaboratoryDidcotUnited KingdomRutherford Appleton Laboratory, Didcot, United Kingdom82Also at School of Physics and Astronomy, University of Southampton, Southampton, United Kingdom.83Also at University of Bristol, Bristol, United Kingdom.R.BainbridgeP.BlochC.E.BrownO.BuchmullerV.CacchioC.A.Carrillo MontoyaG.S.Chahal84D.CollingJ.S.DancuI.DasP.DaunceyG.DaviesJ.DaviesM.Della NegraS.FayerG.FediG.HallM.H.HassanshahiA.HowardG.IlesM.KnightJ.LangfordJ.León HolgadoL.LyonsA.-M.MagnanS.MalikA.MartelliM.MieskolainenJ.Nash85M.PesaresiB.C.Radburn-SmithA.RichardsA.RoseC.SeezR.ShuklaA.TapperK.UchidaG.P.UttleyL.H.VageT.Virdee33M.VojinovicN.WardleD.WinterbottomImperial College, London, United KingdomImperial CollegeLondonUnited KingdomImperial College, London, United Kingdom84Also at IPPP Durham University, Durham, United Kingdom.85Also at Monash University, Faculty of Science, Clayton, Australia.K.ColdhamJ.E.ColeA.KhanP.KyberdI.D.ReidBrunel University, Uxbridge, United KingdomBrunel UniversityUxbridgeUnited KingdomBrunel University, Uxbridge, United KingdomS.AbdullinA.BrinkerhoffB.CarawayJ.DittmannK.HatakeyamaJ.HiltbrandB.McMasterM.SaundersS.SawantC.SutantawibulJ.WilsonBaylor University, Waco, TX, USABaylor UniversityWacoTXUSABaylor University, Waco, Texas, USAR.BartekA.DominguezC.Huerta EscamillaA.E.SimsekR.UniyalA.M.Vargas HernandezCatholic University of America, Washington, DC, USACatholic University of AmericaWashingtonDCUSACatholic University of America, Washington, DC, USAB.BamR.ChudasamaS.I.CooperS.V.GleyzerC.U.PerezP.Rumerio86E.UsaiR.YiThe University of Alabama, Tuscaloosa, AL, USAThe University of AlabamaTuscaloosaALUSAThe University of Alabama, Tuscaloosa, Alabama, USA86Also at Università di Torino, Torino, Italy.A.AkpinarA.AlbertD.ArcaroC.CosbyZ.DemiragliC.EriceC.FangmeierC.Fernandez MadrazoE.FontanesiD.GastlerF.GolfS.JeonI.ReedJ.RohlfK.SalyerD.SperkaD.SpitzbartI.SuarezA.TsatsosS.YuanA.G.ZecchinelliBoston University, Boston, MA, USABoston UniversityBostonMAUSABoston University, Boston, Massachusetts, USAG.BenelliX.Coubez28D.CuttsM.HadleyU.HeintzJ.M.Hogan87T.KwonG.LandsbergK.T.LauD.LiJ.LuoS.MondalM.Narain†N.PervanS.Sagir88F.SimpsonM.StamenkovicW.Y.WongX.YanW.ZhangBrown University, Providence, RI, USABrown UniversityProvidenceRIUSABrown University, Providence, Rhode Island, USA87Also at Bethel University, St. Paul, Minnesota, USA.88Also at Karamanoğlu Mehmetbey University, Karaman, Turkey.S.AbbottJ.BonillaC.BrainerdR.BreedonM.Calderon De La Barca SanchezM.ChertokM.CitronJ.ConwayP.T.CoxR.ErbacherF.JensenO.KukralG.MocellinM.MulhearnD.PellettW.WeiY.YaoF.ZhangUniversity of California, Davis, Davis, CA, USAUniversity of California, DavisDavisCAUSAUniversity of California, Davis, Davis, California, USAM.BachtisR.CousinsA.DattaG.Flores AvilaJ.HauserM.IgnatenkoM.A.IqbalT.LamE.MancaA.Nunez Del PradoD.SaltzbergV.ValuevUniversity of California, Los Angeles, CA, USAUniversity of CaliforniaLos AngelesCAUSAUniversity of California, Los Angeles, California, USAR.ClareJ.W.GaryM.GordonG.HansonW.SiS.Wimpenny†University of California, Riverside, Riverside, CA, USAUniversity of California, RiversideRiversideCAUSAUniversity of California, Riverside, Riverside, California, USAJ.G.BransonS.CittolinS.CoopersteinD.DiazJ.DuarteL.GianniniJ.GuiangR.KansalV.KrutelyovR.LeeJ.LettsM.MasciovecchioF.MokhtarS.MukherjeeM.PieriM.QuinnanB.V.Sathia NarayananV.SharmaM.TadelE.VourliotisF.WürthweinY.XiangA.YagilUniversity of California, San Diego, La Jolla, CA, USAUniversity of California, San DiegoLa JollaCAUSAUniversity of California, San Diego, La Jolla, California, 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USAJ.P.CumalatW.T.FordA.HassaniG.KarathanasisE.MacDonaldN.ManganelliF.MariniA.PerloffC.SavardN.SchonbeckK.StensonK.A.UlmerS.R.WagnerN.ZipperUniversity of Colorado Boulder, Boulder, CO, USAUniversity of Colorado BoulderBoulderCOUSAUniversity of Colorado Boulder, Boulder, Colorado, USAJ.AlexanderS.Bright-ThonneyX.ChenD.J.CranshawJ.FanX.FanD.GadkariS.HoganP.KotamnivesJ.MonroyM.OshiroJ.R.PattersonJ.ReichertM.ReidA.RydJ.ThomP.WittichR.ZouCornell University, Ithaca, NY, USACornell UniversityIthacaNYUSACornell University, Ithaca, New York, USAM.AlbrowM.AlyariO.AmramG.ApollinariA.ApresyanL.A.T.BauerdickD.BerryJ.BerryhillP.C.BhatK.BurkettJ.N.ButlerA.CanepaG.B.CeratiH.W.K.CheungF.ChlebanaG.CummingsJ.DickinsonI.DuttaV.D.ElviraY.FengJ.FreemanA.GandrakotaZ.GecseL.GrayD.GreenA.GrummerS.GrünendahlD.GuerreroO.GutscheR.M.HarrisR.HellerT.C.HerwigJ.HirschauerL.HorynB.JayatilakaS.JindarianiM.JohnsonU.JoshiT.KlijnsmaB.KlimaK.H.M.KwokS.LammelD.LincolnR.LiptonT.LiuC.MadridK.MaeshimaC.MantillaD.MasonP.McBrideP.MerkelS.MrennaS.NahnJ.NgadiubaD.NoonanV.PapadimitriouN.PastikaK.PedroC.Pena89F.RaveraA.Reinsvold Hall90L.RistoriE.Sexton-KennedyN.SmithA.SohaL.SpiegelS.StoynevJ.StraitL.TaylorS.TkaczykN.V.TranL.UpleggerE.W.VaanderingI.ZoiFermi National Accelerator Laboratory, Batavia, IL, USAFermi National Accelerator LaboratoryBataviaILUSAFermi National Accelerator Laboratory, Batavia, Illinois, USA89Also at California Institute of Technology, Pasadena, California, USA.90Also at United States Naval Academy, Annapolis, Maryland, USA.C.ArutaP.AveryD.BourilkovL.CadamuroP.ChangV.CherepanovR.D.FieldE.KoenigM.KolosovaJ.KonigsbergA.KorytovK.H.LoK.MatchevN.MenendezG.MitselmakherK.MohrmanA.Muthirakalayil MadhuN.RawalD.RosenzweigS.RosenzweigK.ShiJ.WangUniversity of Florida, Gainesville, FL, USAUniversity of FloridaGainesvilleFLUSAUniversity of Florida, Gainesville, Florida, USAT.AdamsA.Al KadhimA.AskewN.BowerR.HabibullahV.HagopianR.HashmiR.S.KimS.KimT.KolbergG.MartinezH.ProsperP.R.ProvaO.ViazloM.WulansatitiR.YohayJ.ZhangFlorida State University, Tallahassee, FL, USAFlorida State UniversityTallahasseeFLUSAFlorida State University, Tallahassee, Florida, USAB.AlsufyaniM.M.BaarmandS.ButallaT.Elkafrawy56M.HohlmannR.Kumar VermaM.RahmaniE.YanesFlorida Institute of Technology, Melbourne, FL, USAFlorida Institute of TechnologyMelbourneFLUSAFlorida Institute of Technology, Melbourne, Florida, USAM.R.AdamsA.BatyC.BennettR.CavanaughS.DittmerR.Escobar FrancoO.EvdokimovC.E.GerberD.J.HofmanJ.h.LeeD.S.LemosA.H.MerritC.MillsS.NandaG.OhB.OzekD.PilipovicR.PradhanT.RoyS.RudrabhatlaM.B.TonjesN.VarelasX.WangZ.YeJ.YooUniversity of Illinois Chicago, Chicago, USAUniversity of Illinois ChicagoChicagoUSAUniversity of Illinois Chicago, Chicago, USA, Chicago, USAM.AlhusseiniD.BlendK.Dilsiz91L.EmediatoG.KaramanO.K.KöseyanJ.-P.MerloA.Mestvirishvili92J.NachtmanO.NeogiH.Ogul93Y.OnelA.PenzoC.SnyderE.Tiras94The University of Iowa, Iowa City, IA, USAThe University of IowaIowa CityIAUSAThe University of Iowa, Iowa City, Iowa, USA91Also at Bingol University, Bingol, Turkey.92Also at Georgian Technical University, Tbilisi, Georgia.93Also at Sinop University, Sinop, Turkey.94Also at Erciyes University, Kayseri, Turkey.B.BlumenfeldL.CorcodilosJ.DavisA.V.GritsanL.KangS.KyriacouP.MaksimovicM.RoguljicJ.RoskesS.SekharM.SwartzJohns Hopkins University, Baltimore, MD, USAJohns Hopkins UniversityBaltimoreMDUSAJohns Hopkins University, Baltimore, Maryland, USAA.AbreuL.F.Alcerro AlcerroJ.AnguianoP.BaringerA.BeanZ.FlowersD.GroveJ.KingG.KrintirasM.LazarovitsC.Le MahieuC.LindseyJ.MarquezN.MinafraM.MurrayM.NickelM.PittS.Popescu95C.RoganC.RoyonR.SalvaticoS.SandersC.SmithQ.WangG.WilsonThe University of Kansas, Lawrence, KS, USAThe University of KansasLawrenceKSUSAThe University of Kansas, Lawrence, Kansas, USA95Also at Horia Hulubei National Institute of Physics and Nuclear Engineering (IFIN-HH), Bucharest, Romania.B.AllmondA.IvanovK.KaadzeA.KalogeropoulosD.KimY.MaravinK.NamJ.NatoliD.RoyG.SorrentinoKansas State University, Manhattan, KS, USAKansas State UniversityManhattanKSUSAKansas State University, Manhattan, Kansas, USAF.RebassooD.WrightLawrence Livermore National Laboratory, Livermore, CA, USALawrence Livermore National LaboratoryLivermoreCAUSALawrence Livermore National Laboratory, Livermore, California, USAA.BadenA.BelloniA.BethaniY.M.ChenS.C.EnoN.J.HadleyS.JabeenR.G.KelloggT.KoethY.LaiS.LascioA.C.MignereyS.NabiliC.PalmerC.PapageorgakisM.M.ParanjpeL.WangUniversity of Maryland, College Park, MD, USAUniversity of MarylandCollege ParkMDUSAUniversity of Maryland, College Park, Maryland, USAJ.BendavidW.BuszaI.A.CaliY.ChenM.D'AlfonsoJ.EysermansC.FreerG.Gomez-CeballosM.GoncharovG.GrossoP.HarrisD.HoangD.KovalskyiJ.KrupaL.LavezzoY.-J.LeeK.LongC.MironovC.PausD.RankinC.RolandG.RolandS.RothmanZ.ShiG.S.F.StephansZ.WangB.WyslouchT.J.YangMassachusetts Institute of Technology, Cambridge, MA, USAMassachusetts Institute of TechnologyCambridgeMAUSAMassachusetts Institute of Technology, Cambridge, Massachusetts, USAB.CrossmanB.M.JoshiC.KapsiakM.KrohnD.MahonJ.MansB.MarzocchiS.PandeyM.ReveringR.RusackR.SaradhyN.SchroederN.StrobbeM.A.WadudUniversity of Minnesota, Minneapolis, MN, USAUniversity of MinnesotaMinneapolisMNUSAUniversity of Minnesota, Minneapolis, Minnesota, USAL.M.CremaldiUniversity of Mississippi, Oxford, MS, USAUniversity of MississippiOxfordMSUSAUniversity of Mississippi, Oxford, Mississippi, USAK.BloomM.BrysonD.R.ClaesG.HazaJ.HossainC.JooI.KravchenkoJ.E.SiadoW.TabbA.VagneriniA.WightmanF.YanD.YuUniversity of Nebraska-Lincoln, Lincoln, NE, USAUniversity of Nebraska-LincolnLincolnNEUSAUniversity of Nebraska-Lincoln, Lincoln, Nebraska, USAH.BandyopadhyayL.HayI.IashviliA.KharchilavaM.MorrisD.NguyenS.RappoccioH.Rejeb SfarA.WilliamsState University of New York at Buffalo, Buffalo, NY, USAState University of New York at BuffaloBuffaloNYUSAState University of New York at Buffalo, Buffalo, New York, USAG.AlversonE.BarberisJ.DervanY.HaddadY.HanA.KrishnaJ.LiM.Lu96G.MadiganR.MccarthyD.M.MorseV.NguyenT.OrimotoA.ParkerL.SkinnariA.Tishelman-CharnyB.WangD.WoodNortheastern University, Boston, MA, USANortheastern UniversityBostonMAUSANortheastern University, Boston, Massachusetts, USA96Also at Sun Yat-Sen University, Guangzhou, China.S.BhattacharyaJ.BueghlyZ.ChenK.A.HahnY.LiuY.MiaoD.G.MonkM.H.SchmittA.TaliercioM.VelascoNorthwestern University, Evanston, IL, USANorthwestern UniversityEvanstonILUSANorthwestern University, Evanston, Illinois, USAG.AgarwalR.BandR.BucciS.CastellsA.DasR.GoldouzianM.HildrethK.W.HoK.Hurtado AnampaT.IvanovC.JessopK.LannonJ.LawrenceN.LoukasL.LuttonJ.MarianoN.MarinelliI.McalisterT.McCauleyC.McgradyC.MooreY.Musienko17H.NelsonM.OshersonA.PiccinelliR.RuchtiA.TownsendY.WanM.WayneH.YockeyM.ZaruckiL.ZygalaUniversity of Notre Dame, Notre Dame, IN, USAUniversity of Notre DameNotre DameINUSAUniversity of Notre Dame, Notre Dame, Indiana, USAA.BasnetB.BylsmaM.CarriganL.S.DurkinC.HillM.JoyceM.Nunez OrnelasK.WeiB.L.WinerB.R.YatesThe Ohio State University, Columbus, OH, USAThe Ohio State UniversityColumbusOHUSAThe Ohio State University, Columbus, Ohio, USAF.M.AddesaH.BouchamaouiP.DasG.DezoortP.ElmerA.FrankenthalB.GreenbergN.HaubrichG.KoppS.KwanD.LangeA.LoeligerD.MarlowI.OjalvoJ.OlsenA.ShevelevD.SticklandC.TullyPrinceton University, Princeton, NJ, USAPrinceton UniversityPrincetonNJUSAPrinceton University, Princeton, New Jersey, USAS.MalikUniversity of Puerto Rico, Mayaguez, PR, USAUniversity of Puerto RicoMayaguezPRUSAUniversity of Puerto Rico, Mayaguez, Puerto Rico, USAA.S.BakshiV.E.BarnesS.ChandraR.ChawlaS.DasA.GuL.GutayM.JonesA.W.JungD.KondratyevA.M.KoshyM.LiuG.NegroN.NeumeisterG.PaspalakiS.PiperovV.ScheurerJ.F.SchulteM.StojanovicJ.ThiemanA.K.VirdiF.WangW.XiePurdue University, West Lafayette, IN, USAPurdue UniversityWest LafayetteINUSAPurdue University, West Lafayette, Indiana, USAJ.DolenN.ParasharA.PathakPurdue University Northwest, Hammond, IN, USAPurdue University NorthwestHammondINUSAPurdue University Northwest, Hammond, Indiana, USAD.AcostaT.CarnahanK.M.EcklundP.J.Fernández MantecaS.FreedP.GardnerF.J.M.GeurtsW.LiO.Miguel ColinB.P.PadleyR.RedjimiJ.RotterE.YigitbasiY.ZhangRice University, Houston, TX, USARice UniversityHoustonTXUSARice University, Houston, Texas, USAA.BodekP.de BarbaroR.DeminaJ.L.DulembaC.FallonA.Garcia-BellidoO.HindrichsA.KhukhunaishviliN.ParmarP.Parygin34E.Popova34R.TausG.P.Van OnsemUniversity of Rochester, Rochester, NY, USAUniversity of RochesterRochesterNYUSAUniversity of Rochester, Rochester, New York, USAK.GoulianosThe Rockefeller University, New York, NY, USAThe Rockefeller UniversityNew YorkNYUSAThe Rockefeller University, New York, New York, USAB.ChiaritoJ.P.ChouY.GershteinE.HalkiadakisA.HartM.HeindlD.JaroslawskiO.Karacheban31I.LaflotteA.LathR.MontalvoK.NashH.RoutrayS.SalurS.SchnetzerS.SomalwarR.StoneS.A.ThayilS.ThomasJ.VoraH.WangRutgers, The State University of New Jersey, Piscataway, NJ, USARutgers, The State University of New JerseyPiscatawayNJUSARutgers, The State University of New Jersey, Piscataway, New Jersey, USAH.AcharyaD.AllyA.G.DelannoyS.FiorendiS.HigginbothamT.HolmesA.R.KanugantiN.KarunarathnaL.LeeE.NibigiraS.SpanierUniversity of Tennessee, Knoxville, TN, USAUniversity of TennesseeKnoxvilleTNUSAUniversity of Tennessee, Knoxville, Tennessee, USAD.AebiM.AhmadO.Bouhali97M.DalchenkoR.EusebiJ.GilmoreT.HuangT.Kamon98H.KimS.LuoS.MalhotraR.MuellerD.OvertonD.RathjensA.SafonovTexas A&M University, College Station, TX, USATexas A&M UniversityCollege StationTXUSATexas A&M University, College Station, Texas, USA97Also at Texas A&M University at Qatar, Doha, Qatar.98Also at Kyungpook National University, Daegu, Korea.N.AkchurinJ.DamgovV.HegdeA.HussainY.KazhykarimK.LamichhaneS.W.LeeA.MankelT.PeltolaI.VolobouevA.WhitbeckTexas Tech University, Lubbock, TX, USATexas Tech UniversityLubbockTXUSATexas Tech University, Lubbock, Texas, USAE.AppeltS.GreeneA.GurrolaW.JohnsR.Kunnawalkam ElayavalliA.MeloF.RomeoP.SheldonS.TuoJ.VelkovskaJ.ViinikainenVanderbilt University, Nashville, TN, USAVanderbilt UniversityNashvilleTNUSAVanderbilt University, Nashville, Tennessee, USAB.CardwellB.CoxJ.HakalaR.HiroskyA.LedovskoyC.NeuC.E.Perez LaraUniversity of Virginia, Charlottesville, VA, USAUniversity of VirginiaCharlottesvilleVAUSAUniversity of Virginia, Charlottesville, Virginia, USAP.E.KarchinWayne State University, Detroit, MI, USAWayne State UniversityDetroitMIUSAWayne State University, Detroit, Michigan, USAA.AravindS.BanerjeeK.BlackT.BoseS.DasuI.De BruynP.EveraertsC.GalloniH.HeM.HerndonA.HerveC.K.KorakaA.LanaroR.LovelessJ.Madhusudanan SreekalaA.MallampalliA.MohammadiS.MondalG.ParidaD.PinnaA.SavinV.ShangV.SharmaW.H.SmithD.TeagueH.F.TsoiW.VetensA.WardenUniversity of Wisconsin - Madison, Madison, WI, USAUniversity of Wisconsin - MadisonMadisonWIUSAUniversity of Wisconsin - Madison, Madison, Wisconsin, USAS.AfanasievV.AndreevYu.AndreevT.AushevM.AzarkinA.BabaevA.BelyaevV.Blinov99E.BoosV.BorshchD.BudkouskiV.BunichevV.ChekhovskyR.Chistov99M.Danilov99A.DermenevT.Dimova99D.Druzhkin100M.Dubinin89L.DudkoA.ErshovG.GavrilovV.GavrilovS.GninenkoV.GolovtcovN.GolubevI.GolutvinI.GorbunovA.GribushinY.IvanovV.KachanovV.KarjavineA.KarneyeuV.Kim99M.KirakosyanD.KirpichnikovM.KirsanovV.KlyukhinV.KorenkovA.Kozyrev99N.KrasnikovA.LanevP.Levchenko101N.LychkovskayaV.MakarenkoA.MalakhovV.Matveev99V.MurzinA.Nikitenko102103S.ObraztsovV.OreshkinV.PalichikV.PerelyginM.PerfilovS.Polikarpov99V.PopovO.Radchenko99M.SavinaV.SavrinV.ShalaevS.ShmatovS.ShulhaY.Skovpen99S.SlabospitskiiV.SmirnovD.SosnovV.SulimovE.TcherniaevA.TerkulovO.TeryaevI.TlisovaA.ToropinL.UvarovA.UzunianP.VolkovA.Vorobyev†G.VorotnikovN.VoytishinB.S.Yuldashev104A.ZarubinI.ZhizhinA.ZhokinAuthors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERNAuthors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERNAuthors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN99Also at another institute or international laboratory covered by a cooperation agreement with CERN.100Also at Universiteit Antwerpen, Antwerpen, Belgium.101Also at Northeastern University, Boston, Massachusetts, USA.102Also at Imperial College, London, United Kingdom.103Now at Yerevan Physics Institute, Yerevan, Armenia.104Also at Institute of Nuclear Physics of the Uzbekistan Academy of Sciences, Tashkent, Uzbekistan.CERN, Geneva, SwitzerlandCERNGenevaSwitzerlandCERN, Geneva, Switzerland⋆E-mail address:cms-publication-committee-chair@cern.ch.Editor: M. DoserAbstractA search is presented for new Higgs bosons in proton-proton (pp) collision events in which a same-sign top quark pair is produced in association with a jet, via the pp→tH/A→ttc‾ and pp→tH/A→ttu‾ processes. Here, H and A represent the extra scalar and pseudoscalar boson, respectively, of the second Higgs doublet in the generalized two-Higgs-doublet model (g2HDM). The search is based on pp collision data collected at a center-of-mass energy of 13 TeV with the CMS detector at the LHC, corresponding to an integrated luminosity of 138fb−1. Final states with a same-sign lepton pair in association with jets and missing transverse momentum are considered. New Higgs bosons in the 200–1000 GeV mass range and new Yukawa couplings between 0.1 and 1.0 are targeted in the search, for scenarios in which either H or A appear alone, or in which they coexist and interfere. No significant excess above the standard model prediction is observed. Exclusion limits are derived in the context of the g2HDM.KeywordsCMSTop quarksExtra Higgs bosonYukawa couplingsData availabilityRelease and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS policy as stated in “CMS data preservation, re-use and open access policy”.1IntroductionUsing proton-proton (pp) collision data recorded during the CERN LHC Run 1 (2011–2012) data-taking period, the ATLAS and CMS experiments discovered a scalar boson, h125, with a mass of 125 GeV, the properties of which are so far consistent with those of the Higgs boson of the standard model (SM) [1–3]. The analysis of the additional Run 2 (2015–2018) data enabled more precise measurements of the Higgs boson properties and further constrained the possible contributions from new physics beyond the SM [4,5]. The ATLAS and CMS experiments have measured the Yukawa couplings of the h125 boson to the t and b quarks, and the τ and μ leptons [6,7]. In all cases, the couplings are found to be consistent with the SM expectations within uncertainties.Having established the existence of one scalar SU(2) doublet, natural questions emerge about the possibility of additional doublets. A second doublet is predicted in two-Higgs-doublet models (2HDM), resulting in five physical scalar bosons: CP-even neutral scalar bosons h and H with mH>mh, a CP-odd pseudoscalar boson A, and two charged Higgs bosons H±[8]. These additional Higgs bosons at mass scales ≲1TeV may still exist within the reach of the LHC [9], but their signatures may be suppressed by fermion mass-mixing hierarchy [10] or alignment mechanisms, where the mixing angle γ between the two CP-even scalar bosons h and H has a value for which cos⁡γ≈0[11]. In the alignment limit [12–14], the lightest scalar boson h becomes the SM h125 boson, and the extra spin-0 bosons do not interact with vector boson pairs (i.e., HVV and AVV interactions do not occur, where V is a W or Z boson). Alignment suppresses flavor changing neutral current interactions of the h boson but allows them for the H and A bosons. Therefore, the lack of a hint of the processes such as t→ch125/uh125 or h125→μτ/eτ at the LHC may be because their amplitudes are suppressed by alignment. As shown in Ref. [11], the alignment scenario may occur if all extra Higgs quartic couplings are O(1) and no Z2 symmetry requirement is imposed, allowing flavor changing neutral Higgs couplings involving H and A bosons. This scenario without Z2 symmetry can be studied in the framework of the generalized 2HDM (g2HDM) [8,10,15], with new Yukawa couplings such as ρτμ, ρtu, ρtc, and ρtt that may assume significantly large values [8,10,15]. These new Yukawa couplings combined with Higgs quartic couplings of ≈1 may also explain the electroweak baryogenesis [16,17] and therefore the disappearance of antimatter soon after the Big Bang. The new top Yukawa coupling ρtc with a similar strength to ρτμ may be compatible with the observed data depending on the H± mass, which may also explain a possible muon g−2 anomaly [18]. These arguments strongly motivate to verify with direct experimental searches whether new Yukawa couplings exist. The processes discussed above have been recently explored by the ATLAS experiment [19].In this Letter, we present a search for the existence of the real part of these couplings, ρtu and ρtc, through the pp→tH/A→ttq‾(q=u,c) and the charge conjugate processes, considering one coupling at a time and keeping the other at zero using the Run 2 data set recorded by the CMS experiment. A representative Feynman diagram for the ttq‾ process is displayed in Fig. 1. The final-state signature for ttq‾ explored in this Letter consists of two same-sign (SS) leptons with at least three jets, two of which are identified as b jets and one compatible with originating from a u or c quark, and missing transverse momentum. The main background consists of events with nonprompt leptons originating from leptonic decays of heavy quarks, hadrons misidentified as leptons, electrons from photon conversions, or jets misidentified as leptons.The analysis is performed using pp collision data at a center-of-mass energy of 13 TeV. The data were collected with the CMS detector at the LHC between 2016 and 2018, and correspond to an integrated luminosity of 138fb−1. Tabulated results are accessible from the HEPData record for this analysis [20].The Letter is organized as follows: Section 2 describes the CMS detector, along with object reconstruction. In Section 3, a description of the simulation samples used in the analysis is given. The event selection and reconstruction procedure of the physics objects are given in Section 4. Following, in Section 5, the signal extraction procedure is explained. Section 6 discusses the sources of systematic uncertainties. The results of the analysis are presented in Section 7. Finally, a summary of the analysis is given in Section 8.2The CMS detector and object reconstructionThe CMS apparatus [21] is a multipurpose, nearly hermetic detector, designed to trigger on [22,23] and identify electrons, muons, photons, and (charged and neutral) hadrons [24–26]. A global “particle-flow” (PF) algorithm [27] aims to reconstruct all individual particles in an event, combining information provided by the all-silicon inner tracker and by the crystal electromagnetic (ECAL) and brass-scintillator hadron calorimeters (HCAL), operating inside a 3.8 T superconducting solenoid, with data from the gas-ionization muon detectors embedded in the flux-return yoke outside the solenoid.The primary vertex is taken to be the vertex corresponding to the hardest scattering in the event, evaluated using tracking information alone, as described in Section 9.4.1 of Ref. [28]. The energy of photons is obtained from the ECAL measurement. The energy of electrons is determined from a combination of the electron momentum at the primary interaction vertex as determined by the tracker, the energy of the corresponding ECAL cluster, and the energy sum of all bremsstrahlung photons spatially compatible with originating from the electron track. The energy of muons is obtained from the curvature of the corresponding track. The energy of charged hadrons is determined from a combination of their momentum measured in the tracker and the matching ECAL and HCAL energy deposits, corrected for the response function of the calorimeters to hadronic showers. Finally, the energy of neutral hadrons is obtained from the corresponding corrected ECAL and HCAL energies.Jets are built from PF particles using the anti-kT algorithm [29,30] with a distance parameter of 0.4. Jet momentum is determined as the vectorial sum of all particle momenta in the jet, and is found from simulation to be, on average, within 5 to 10% of the true momentum over the whole pT spectrum and detector acceptance. Additional pp interactions within the same or nearby bunch crossings can contribute additional tracks and calorimetric energy depositions, increasing the apparent jet momentum. To mitigate this effect, tracks identified to be originating from the multiple pp interactions occurring in the same or nearby bunch crossings (pileup) are discarded and an offset correction is applied to correct for remaining contributions [31]. Jet energy corrections are derived from simulation studies so that the average measured energy of jets becomes identical to that of particle level jets. In situ measurements of the momentum balance in dijet, photon+jet, Z+jets, and multijet events are used to determine any residual differences between the jet energy scale in data and in simulation, and appropriate corrections are made [32]. Additional selection criteria are applied to each jet to remove jets potentially dominated by instrumental effects or reconstruction failures [31]. The missing transverse momentum vector p→Tmiss is computed as the negative vector sum of the transverse momenta of all the PF candidates in an event, and its magnitude is denoted as pTmiss[33]. The p→Tmiss is modified to account for corrections to the energy scale of the reconstructed jets in the event.Events of interest are selected using a two-tiered trigger system. The first level (L1), composed of custom hardware processors, uses information from the calorimeters and muon detectors to select events at a rate of around 100 kHz within a fixed latency of about 4μs[22]. The second level, known as the high-level trigger, consists of a farm of processors running a version of the full event reconstruction software optimized for fast processing, and reduces the event rate to around 1 kHz before data storage [23].3Simulated event samplesThe signal and background processes are simulated using several Monte Carlo (MC) programs. The ttq‾ signal samples are simulated at leading order (LO) in perturbative quantum chromodynamics (QCD) with up to two additional noncollinear high-pT partons using MadGraph5_amc@nlo 2.6.5 [34], and the hard-process simulation is interfaced with parton shower jets using the MLM [35] matching prescription. Different signal samples are simulated for the case where a mass between 200 and 1000 GeV is assumed for A (H), and a mass too high to be of reach for our search is assumed for H (A). For these signal samples, there is no interference between A and H. Signal samples are also generated for the case where both A and H coexist and interfere assuming a mass difference mA−mH=50GeV, following Ref. [36]. The amplitudes for the processes qg→tA→ttq‾ and qg→tH→ttq‾ cancel when A and H are mass degenerate. The signal cross section is not significantly modified with respect to the noninterference case when the mass differences are larger than ≈100GeV. Therefore, the investigated mass difference is chosen to retain some interference effects along with reasonably high cross sections. Depending on the coupling value and the interference assumption we consider in this Letter, the cross sections for the ttu‾ process range from ≈1×10−4 to ≈7×10−1pb and for ttc‾ range from ≈5×10−6 to ≈7×10−2pb, as calculated with MadGraph5_amc@nlo at LO precision in QCD. The inclusive cross section for the ttq‾ process does not change, within uncertainties, when the intermediary particle is H or A, when there is no A-H interference.Background events generated by the MadGraph5_amc@nlo generator are tt‾V, V+jets, tt‾VV, tt‾VH, tZ, tt‾tj, tt‾tW, tt‾tt‾, WZ, vector boson scattering (VBS, i.e., Wℓℓqq or V±V±JJ), VVV, and single top quark s-channel production. Among these processes, FxFx matching [37] is used for tt‾W, Z+jets, and the QCD part of WZ production, while MLM matching [35] is used for W+jets. The powheg 2.0 generator [38–40] is used to simulate events at next-to-LO in perturbative QCD for tt‾[41], ZZ and W±W∓[42], single top quark tW [43] and t-channel [44], and tt‾H production [45].Both the signal and background samples are interfaced with pythia v8.240 [46] for parton showering, fragmentation, and hadronization. The underlying event is also modeled with pythia, using the CP5 tune [47]. The parton distribution functions (PDFs) are taken from the NNPDF3.1 next-to-next-to-LO set [48]. Finally, for both signal and background MC event samples, the detector response is modeled with the Geant4 package [49]. The simulated events are weighted to match the observables sensitive to pileup to those observed in the data [31].The simulated events are corrected for the differences between data and simulation of the trigger efficiencies, lepton identification, and lepton isolation. The corrections are determined using the “tag-and-probe” method applied on Z boson candidate events [50] and are parametrized as functions of the lepton pT and pseudorapidity (η).4Event reconstruction and selectionData are selected online with a combination of double lepton triggers and single lepton triggers to enhance signal efficiency. Charged leptons (electrons or muons) are required to originate from the primary vertex to reject contributions from pileup. Identification of electrons makes use of a multivariate discriminant [51,52] combining observables sensitive to the matching of charged-particle tracks in the tracker to the energy deposits in the ECAL and the amount of bremsstrahlung photons emitted along their trajectory [24]. The number of electrons originating from asymmetric photon conversions is reduced by requiring that their associated track has no missing hits in the innermost layers of the silicon tracker. To ensure the correct assignment of the electric charge of the electrons, further selection criteria were applied [53]. The separation of prompt leptons from nonprompt leptons reconstructed within jets is achieved by using an isolation variable, relative to the lepton pT. The isolation variable is constructed from the scalar pT sum of charged hadrons, neutral hadrons, and photons reconstructed within a cone of variable size that depends on the lepton pT[54]. “Loose” leptons are those that pass the kinematic selection criteria of pT>10GeV and |η|<2.5(2.4) for electrons (muons). Electrons that fall in the region between the ECAL barrel and endcaps (1.442<|η|<1.556) are vetoed. “Tight” leptons are in addition required to have pT>20GeV. A multivariate discriminant is furthermore used to separate prompt leptons and nonprompt leptons originating from the decays of hadrons inside jets, hadrons misidentified as leptons, and electrons from photon conversions. The jets must have pT>30GeV and |η|<2.4 to be considered. In addition, they are required to be separated from identified leptons by ΔR=(Δη)2+(Δϕ)2>0.4, where ϕ is the azimuthal angle measured in radians. At least three jets, and pTmiss>30GeV are required in each event. Jets from the hadronization of b quarks (b jets), c quarks (c jets), and light (i.e., light-quark or gluon) jets are distinguished through the ratios of the corresponding jet flavor probabilities, defined as CvsL (c vs light quark) and CvsB (c vs b quark) [55,56], respectively. These probabilities are obtained from the DeepJet[57,58] algorithm: a neural network utilizing global variables, charged, neutral particle and secondary vertex features in a jet to perform flavor tagging. The differences of the shapes of the CvsL and CvsB discriminant distributions between data and simulation are corrected by flavor-dependent scale factors.The search is performed in three SS dilepton categories: e±e±, μ±μ±, and e±μ±. The event selection ensures complete orthogonality of these three categories to avoid any possible double counting of events selected in the analysis. Events are required to have two tight leptons with the same electric charge for which the leading lepton has pT>30GeV and subleading lepton pT>20GeV. Events containing a third lepton are vetoed if the additional lepton passes the loose selection. The two leptons are required to be separated by ΔR(ℓ1,ℓ2)>0.3 and required to have an invariant mass m(ℓ1,ℓ2)>20GeV. Events with 60<m(ℓ1,ℓ2)<120GeV in the e±e± channel are vetoed to suppress the Drell-Yan (DY) background contribution, the main source of charge misidentified leptons. This veto reduces the selected number of DY events in simulation by about 94% after the aforementioned requirements. This veto is not applied to the e±μ± and μ±μ± channels, as the charge misidentification rate for muons is negligible. The CvsL and CvsB distributions for the leading jet obtained from simulated events and data are displayed in Fig. 2.The nonprompt-lepton background is estimated from control regions in the data using the fake-factor method [59]. A dijet enriched sample is selected from data, from which the probability fp for a loose nonprompt lepton (originating from a jet) to also pass the tight lepton selection criteria is estimated in bins of pT and |η|. The nonprompt-lepton background contribution is then estimated by applying fp to events in a data control sample in which at least one lepton fails the tight lepton selection criteria. A data-driven approach is followed to evaluate the lepton charge misidentification rate in the e±e± channel using DY events with same- and opposite-sign electric charges. It is estimated in bins of lepton pT and η, and is used to calibrate simulated events. The rate, which increases with pT and η, varies from ≈10−5 to ≈10−2.5Signal extractionA boosted decision tree (BDT) discriminant [60] is used to separate signal and background events. We train the BDT model in the signal region, where process yields of both backgrounds and signal are small. For the training, we combine the inputs from different channels. By comparing the BDT output distributions for the training and test samples, we found no evidence of overtraining. We use an optimized set of input observables, listed in Table 1, for our signal topology. Flavor tagging variables are used to differentiate b quarks originating from the top quark decay, and to differentiate c quark and light-quark jets. Pairwise kinematic variables related to jets are incorporated that are sensitive to the resonance structures, specifically to top quarks and A/H. Other kinematic features, such as HT and pTmiss, are also sensitive to our signal and are included. To mitigate the impact of resonances such as the DY process, the dilepton (+jets) invariant mass is also used as an input to the BDT.We use half of the available simulated events for the BDT training. The main backgrounds in the signal region are tt‾ (fully leptonic decay of the top quark-antiquark pair where one lepton has a misidentified charge), nonprompt leptons (dominated by semileptonic tt‾ decay), tt‾W, and tt‾H. In the signal extraction, we use events from data to estimate the nonprompt-lepton background contribution, but we do not use these events for training. Instead, we use simulated samples of semileptonically decaying tt‾ events for the BDT training, to mimic the misidentified lepton in the nonprompt-lepton background. We do not include events from W+jets or single top quark simulation, due to a limited number of simulated events. The various backgrounds are added corresponding to their cross sections. The MC event samples used for the BDT training are ttc‾ or ttu‾ signal, semileptonic tt‾, dileptonic tt‾ (tt‾), tt‾V, VV, VVV, tt‾H, tt‾VH, tt‾VV, tt‾tj, tt‾tW, tt‾tt‾, and VBS. Three values for the couplings ρtu and ρtc, namely, 0.1, 0.4, and 1.0 are considered. For each coupling, ten mA points are considered: 200, 300, 350, 400, 500, 600, 700, 800, 900, and 1000 GeV. Using the same coupling assumptions, we also consider the more realistic case with the A-H interference assuming a fixed mass difference mA−mH=50GeV, with the following nine mA-mH combinations; 250-200, 300-250, 350-300, 400-350, 550-500, 700-650, 800-750, 900-850, and 1000-950 GeV. The signal extraction is performed using the shape of the BDT discriminant distributions. Because of the kinematic differences and different background compositions, the BDTs are trained independently for four data-taking periods, two in 2016, and one for each of the years 2017 and 2018; for each mass assumption, namely for each mA either with no H present or with A-H interference; and for ρtu=0.4 and ρtc=0.4. Therefore, a total of 152 BDTs are trained. The values of the BDT hyperparameters, as defined in the TMVA package [61], are chosen after scanning a range of values, avoiding overtraining, and requiring a high background rejection rate while maintaining a high signal efficiency. We use these same model parameters for all three years of data taking. The BDTs offer high background rejection, while simultaneously maintaining a high signal efficiency. For instance, when considering ρtc=0.4, and a signal efficiency of 96%, the background rejection rates for mA=200GeV and 1000GeV are 50% and 76%, respectively.The signal strength parameter, μ, is obtained using a simultaneous maximum likelihood fit [62], in analyses performed for three decay modes and for four different eras (i.e. 12 categories) for each signal mass-coupling assumption independently. It is defined as μ=σ/σtheory, where σtheory is the predicted ttq‾ production cross section in g2HDM calculated with MadGraph5_amc@nlo +pythia, and σ is the upper limit on the observed cross section. To ensure numerical stability, the bin width is chosen to have a high enough yield in each bin of the BDT distributions. The BDT distribution ranges from −1 to 1, but to reduce the impact on the fit of background-dominated regions, events are selected with a BDT score >−0.6. This requirement on the BDT score also helps to improve the stability of the fit and the corresponding fit uncertainties. Except for the dominant nonprompt-lepton background, the predicted yields and the shapes of the BDT distributions are taken directly from the simulation. When performing the maximum likelihood fit, individual templates are used for the VBS, VV, tt‾ (fully leptonic decays), tt‾H, tt‾W, and nonprompt-lepton background processes, while a combined template labeled others uses a combination of background processes, namely: DY, tt‾VV, tt‾VH, tt‾Z, tt‾tj, tt‾tW, tt‾tt‾, VVV, tZq, tW, and t‾W.6Systematic uncertaintiesSystematic uncertainties, arising from various sources, such as detector effects, theoretical uncertainties, and mismodeling, are evaluated and categorized in two main groups: experimental uncertainties and modeling uncertainties. Several effects modify the event yields or shapes of the measured distributions. The systematic uncertainties are modeled as nuisance parameters in the maximum likelihood estimation procedure used for determining the best fit signal strength μˆ. The nuisance parameters are allowed to modify the shape and normalization of the backgrounds and signal in the fit using the method in Ref. [62]. The chosen probability density function (pdf) used for the interpolation between nominal and systematic templates is dependent on whether the associated nuisance parameter can also affect the shape of the nominal template or not. Log-normal pdfs are used for nuisance parameters that only affect the distributions normalization, whereas Gaussian distributions are used for those that can affect the shape as well. Experimental uncertainties, where appropriate, and all modeling uncertainties are taken as correlated across years and channels. The effect of the limited number of simulated events is estimated using the Barlow–Beeston-lite method [63].The experimental uncertainties are those related to the integrated luminosity [64–66], pileup, L1 trigger inefficiency, nonprompt-lepton background estimation, jet energy scale and resolution, unclustered energy scale, lepton identification and trigger efficiencies, charge misidentification, muon momentum scale, and heavy-quark, light-quark and gluon jet identification. The dominant experimental uncertainty sources are related to the flavor tagger discriminant shape calibration, and nonprompt-lepton background estimation. The modeling uncertainty sources are matrix-element renormalization and factorization scales, parton shower scales that control the initial- and final-state radiation, and PDFs. For the signal, these are included as separate nuisance parameters that affect the shape. For the backgrounds estimated using MC event samples, nuisance parameters are assumed to only affect the yields, and the corresponding uncertainties in the theoretical cross section calculations are used. The most significant modeling uncertainty in the analysis is attributed to the normalization of the tt‾W background, regardless of the A-H interference. The contributions of all uncertainty sources on the pre-fit expected event yields are displayed in Table 2, for ρtc=0.4 and mA=350GeV with A-H interference assuming mA−mH=50GeV. The uncertainties in other scenarios are similar.7ResultsFig. 3 displays the post-fit BDT discriminant distributions used for the signal extraction combining the categories e±e±, μ±μ±, and e±μ±, and for ρtu=1.0 and ρtc=1.0 with A-H interference, assuming mA=350GeV.No significant excess over the expected SM background is observed. The results of the search are interpreted in terms of the upper limits on the signal strength parameter μ in the g2HDM. The upper limits on μ are calculated at 95% confidence level (CL) using a modified frequentist method [67–69] computed with an asymptotic approximation [70]. The expected 95% CL on the production cross section and the regions containing 68 and 95% of the distribution of the limits expected under the background-only hypothesis are calculated with pseudo-experiments using background-only samples. It is observed that the shapes of the BDT distributions are consistent with each other for different coupling values at the same A or H mass value. Therefore, for other coupling assumptions than ρtu/tc=0.4, the expected signal yields are scaled separately for ρtu and ρtc for each mass and coupling hypothesis making use of the corresponding signal cross sections. It is also observed that A or H can be used interchangeably as their corresponding BDT distribution shapes as well as their cross sections are the same. Therefore, we only show the results for A in this Letter. The observed and expected upper limits are displayed as functions of mA from 200 to 1000 GeV for ρtu=0.1,0.4,1.0 and ρtc=0.1,0.4,1.0, for the Run-2 data and for the combination of all three decay modes, without (with) A-H interference in Fig. 4(5). The observed limits at 95% CL on the signal strength as functions of mA and the new Yukawa couplings ρtc/tu are shown in Fig. 6 without A-H interference, and in Fig. 7 with A-H interference. Interpreted in g2HDM, exclusion limits at 95% CL on the mass of the additional Higgs bosons A and H are shown in Table 3 for different ρtu and ρtc assumptions.8SummaryA search for new Yukawa couplings of the top quark in models with additional Higgs bosons in proton-proton collisions at a center-of-mass energy of 13 TeV has been presented. The process considered is the production of same-sign top quark pairs associated with an up or a charm quark, and resulting in a final state containing two same-sign leptons and jets. No significant excess above the background prediction is observed. When no interference between the pseudoscalar (A) and scalar (H) Higgs bosons is assumed, A or H bosons with masses below 920 GeV and 1000 GeV are excluded at the 95% confidence level (CL) for coupling values ρtu=0.4 and 1.0, respectively, while all other extra Yukawa couplings are assumed to be zero. Similarly, without interference between H and A, and assuming a coupling value of ρtc=1.0, A or H bosons with masses below approximately 770GeV are excluded at the 95% CL. Under the assumption that A and H interfere in the scenario with a mass difference of mA−mH=50GeV, the pseudoscalar Higgs boson is excluded for mA values below 1000GeV when considering coupling values ρtu>0.4. Furthermore, assuming ρtc=0.4, the exclusion limit for A is mA=340GeV, whereas assuming ρtc=1.0, the limit extends to mA=810GeV at 95% CL. These results represent the first search based on the generalized two-Higgs-doublet model considering A-H interference.Declaration of Competing InterestThe authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.AcknowledgementsWe congratulate our colleagues in the CERN accelerator departments for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their contributions to the success of the CMS effort. In addition, we gratefully acknowledge the computing centers and personnel of the Worldwide LHC Computing Grid and other centers for delivering so effectively the computing infrastructure essential to our analyses. Finally, we acknowledge the enduring support for the construction and operation of the LHC, the CMS detector, and the supporting computing infrastructure provided by the following funding agencies: SC (Armenia), BMBWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, FAPERGS, and FAPESP (Brazil); MES and BNSF (Bulgaria); CERN; CAS, MOST, and NSFC (China); Minciencias (Colombia); MSES and CSF (Croatia); RIF (Cyprus); SENESCYT (Ecuador); MoER, ERC PUT and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); SRNSF (Georgia); BMBF, DFG, and HGF (Germany); GSRI (Greece); NKFIH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); MSIP and NRF (Republic of Korea); MES (Latvia); LAS (Lithuania); MOE and UM (Malaysia); BUAP, CINVESTAV, CONACYT, LNS, SEP, and UASLP-FAI (Mexico); MOS (Montenegro); MBIE (New Zealand); PAEC (Pakistan); MES and NSC (Poland); FCT (Portugal); MESTD (Serbia); MCIN/AEI and PCTI (Spain); MoSTR (Sri Lanka); Swiss Funding Agencies (Switzerland); MST (Taipei); MHESI and NSTDA (Thailand); TUBITAK and TENMAK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA).Individuals have received support from the Marie-Curie program and the European Research Council and Horizon 2020 Grant, contract Nos. 675440, 724704, 752730, 758316, 765710, 824093, and COST Action CA16108 (European Union); the Leventis Foundation; the Alfred P. Sloan Foundation; the Alexander von Humboldt Foundation; the Science Committee, project no. 22rl-037 (Armenia); the Belgian Federal Science Policy Office; the Fonds pour la Formation à la Recherche dans l'Industrie et dans l'Agriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); the F.R.S.-FNRS and FWO (Belgium) under the “Excellence of Science – EOS” – be.h project n. 30820817; the Beijing Municipal Science & Technology Commission, No. Z191100007219010 and Fundamental Research Funds for the Central Universities (China); The Ministry of Education, Youth and Sports (MEYS) of the Czech Republic; the Shota Rustaveli National Science Foundation, grant FR-22-985 (Georgia); the Deutsche Forschungsgemeinschaft (DFG), under Germany's Excellence Strategy – EXC 2121 “Quantum Universe” – 390833306, and under project number 400140256 - GRK2497; the Hellenic Foundation for Research and Innovation (HFRI), Project Number 2288 (Greece); the Hungarian Academy of Sciences, the New National Excellence Program - ÚNKP, the NKFIH research grants K 124845, K 124850, K 128713, K 128786, K 129058, K 131991, K 133046, K 138136, K 143460, K 143477, 2020-2.2.1-ED-2021-00181, and TKP2021-NKTA-64 (Hungary); the Council of Science and Industrial Research, India; ICSC – National Research Center for High Performance Computing, Big Data and Quantum Computing, funded by the EU NexGeneration program (Italy); the Latvian Council of Science; the Ministry of Education and Science, project no. 2022/WK/14, and the National Science Center, contracts Opus 2021/41/B/ST2/01369 and 2021/43/B/ST2/01552 (Poland); the Fundação para a Ciência e a Tecnologia, grant CEECIND/01334/2018 (Portugal); the National Priorities Research Program by Qatar National Research Fund; MCIN/AEI/10.13039/501100011033, ERDF “a way of making Europe”, and the Programa Estatal de Fomento de la Investigación Científica y Técnica de Excelencia María de Maeztu, grant MDM-2017-0765 and Programa Severo Ochoa del Principado de Asturias (Spain); the Chulalongkorn Academic into Its 2nd Century Project Advancement Project, and the National Science, Research and Innovation Fund via the Program Management Unit for Human Resources & Institutional Development, Research and Innovation, grant B05F650021 (Thailand); the Kavli Foundation; the Nvidia Corporation; the SuperMicro Corporation; the Welch Foundation, contract C-1845; and the Weston Havens Foundation (USA).References[1]ATLAS CollaborationObservation of a new particle in the search for the standard model Higgs boson with the ATLAS detector at the LHCPhys. 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The search is based on pp collision data collected at a center-of-mass energy of 13 TeV with the CMS detector at the LHC, corresponding to an integrated luminosity of 138fb\u22121. Final states with a same-sign lepton pair in association with jets and missing transverse momentum are considered. New Higgs bosons in the 200\u20131000 GeV mass range and new Yukawa couplings between 0.1 and 1.0 are targeted in the search, for scenarios in which either H or A appear alone, or in which they coexist and interfere. No significant excess above the standard model prediction is observed. Exclusion limits are derived in the context of the g2HDM." + }, + "authors": [ + { + "affiliation": [ + { + "affPubRaw": "Yerevan Physics Institute, Yerevan, Armenia" + } + ], + "name": { + "given_name": "A.", + "surname": "Hayrapetyan" + } + }, + { + "affiliation": [ + { + "affPubRaw": "Also at Yerevan State University, Yerevan, Armenia." + } + ], + "attrib": { + "orcid": "0009-0000-0684-6742" + }, + "name": { + "given_name": "A.", + "surname": "Tumasyan" + } + }, + { + "affiliation": [ + { + "affPubRaw": "Institut f\u00fcr Hochenergiephysik, Vienna, Austria" + } + ], + "attrib": { + "orcid": "0000-0001-9099-4341" + }, + "name": { + "given_name": "W.", + "surname": "Adam" + } + }, + { + "affiliation": [ + { + "affPubRaw": "Institut f\u00fcr Hochenergiephysik, Vienna, Austria" + } + ], + "name": { + "given_name": "J.W.", + "surname": "Andrejkovic" + } + }, + { + "affiliation": [ + { + "affPubRaw": "Institut f\u00fcr Hochenergiephysik, Vienna, Austria" + } + ], + "attrib": { + "orcid": 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C712011155410.1140/epjc/s10052-011-1554-0arXiv:1007.1727Erratum:https://doi.org/10.1140/epjc/s10052-013-2501-z" + ], + "title": { + "textEnglish": "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at s=13TeV" + } +} diff --git a/tests/test_elsevier.py b/tests/test_elsevier.py index a66b674..260dabb 100644 --- a/tests/test_elsevier.py +++ b/tests/test_elsevier.py @@ -34,6 +34,7 @@ def test_elsevier(self): "els_detag_example_1", "els_detag_example_2", "els_list", + "els_phlb_compound_affil", ] for f in filenames: test_infile = os.path.join(self.inputdir, f + ".xml") From 8e8759e5d2a3ac71a44a7a770b1fe86a5678293b Mon Sep 17 00:00:00 2001 From: Matthew Templeton Date: Sat, 27 Apr 2024 13:17:51 -0400 Subject: [PATCH 07/10] Affs need to have all sources, not one or the other modified: adsingestp/parsers/elsevier.py --- adsingestp/parsers/elsevier.py | 8 ++++---- 1 file changed, 4 insertions(+), 4 deletions(-) diff --git a/adsingestp/parsers/elsevier.py b/adsingestp/parsers/elsevier.py index 4492e33..dbb35c8 100644 --- a/adsingestp/parsers/elsevier.py +++ b/adsingestp/parsers/elsevier.py @@ -317,16 +317,16 @@ def _parse_author_group(self, author_group): and author.find("ce:e-address").get("type", "") == "email" ): author_tmp["email"] = author.find("ce:e-address").get_text() + affs = [] + if affs_xref.get("ALLAUTH"): + affs.append(affils_xref.get("ALLAUTH")) if author.find("ce:cross-ref") and author.find("ce:cross-ref").find("sup"): - affs = [] for i in author.find("ce:cross-ref").find_all("sup"): aff_label = i.get_text() # don't append an empty aff if affs_xref.get(aff_label): affs.append(affs_xref[aff_label]) - author_tmp["aff"] = affs - elif affs_xref.get("ALLAUTH"): - author_tmp["aff"] = affs_xref["ALLAUTH"] + author_tmp["aff"] = affs group_author_list.append(author_tmp) return group_author_list From db228406aa29347bfbd0ee7188a38d18b7902aba Mon Sep 17 00:00:00 2001 From: Matthew Templeton Date: Sat, 27 Apr 2024 13:58:47 -0400 Subject: [PATCH 08/10] Mod correctly captures affils for other test cases modified: adsingestp/parsers/elsevier.py modified: tests/stubdata/input/els_phlb_compound_affil.xml modified: tests/stubdata/output/els_book_review.json modified: tests/stubdata/output/els_phlb_compound_affil.json modified: tests/stubdata/output/els_simple_article_3.json modified: tests/stubdata/output/els_simple_article_4.json --- adsingestp/parsers/elsevier.py | 9 +- .../input/els_phlb_compound_affil.xml | 2 +- tests/stubdata/output/els_book_review.json | 5 + .../output/els_phlb_compound_affil.json | 503 ++++++++++++++++++ .../stubdata/output/els_simple_article_3.json | 5 + .../stubdata/output/els_simple_article_4.json | 5 + 6 files changed, 523 insertions(+), 6 deletions(-) diff --git a/adsingestp/parsers/elsevier.py b/adsingestp/parsers/elsevier.py index dbb35c8..d9d891a 100644 --- a/adsingestp/parsers/elsevier.py +++ b/adsingestp/parsers/elsevier.py @@ -17,8 +17,8 @@ def flatten_author_groups(soup): # returning a list of flat author groups # without any embedded groups group_list = [] - ag = soup.find('ce:author-group').extract() - while ag.find('ce:author-group'): + ag = soup.find("ce:author-group").extract() + while ag.find("ce:author-group"): group_list.append(flatten_author_groups(ag)) g2 = [ag] g2.extend(group_list) @@ -31,7 +31,6 @@ def flatten_author_groups(soup): return group_list - class ElsevierParser(BaseBeautifulSoupParser): author_collaborations_params = {} @@ -300,7 +299,7 @@ def _parse_author_group(self, author_group): affs_xref["ALLAUTH"] = value_list else: affs_xref[label] = value - + authors_raw = author_group.find_all("ce:author") for author in authors_raw: author_tmp = {} @@ -319,7 +318,7 @@ def _parse_author_group(self, author_group): author_tmp["email"] = author.find("ce:e-address").get_text() affs = [] if affs_xref.get("ALLAUTH"): - affs.append(affils_xref.get("ALLAUTH")) + affs.extend(affs_xref.get("ALLAUTH")) if author.find("ce:cross-ref") and author.find("ce:cross-ref").find("sup"): for i in author.find("ce:cross-ref").find_all("sup"): aff_label = i.get_text() diff --git a/tests/stubdata/input/els_phlb_compound_affil.xml b/tests/stubdata/input/els_phlb_compound_affil.xml index 5686580..db57415 100644 --- a/tests/stubdata/input/els_phlb_compound_affil.xml +++ b/tests/stubdata/input/els_phlb_compound_affil.xml @@ -1 +1 @@ -application/xmlSearch for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at [formula omitted]The CMS CollaborationA. HayrapetyanA. TumasyanW. AdamJ.W. AndrejkovicT. BergauerS. ChatterjeeK. DamanakisM. DragicevicP.S. HussainM. JeitlerN. KrammerA. LiD. LikoI. MikulecJ. SchieckR. SchöfbeckD. SchwarzM. SonawaneS. TemplW. WaltenbergerC.-E. WulzM.R. DarwishT. JanssenP. Van MechelenE.S. BolsJ. D'HondtS. DansanaA. De MoorM. DelcourtH. El FahamS. LowetteI. MakarenkoD. MüllerA.R. SahasransuS. TavernierM. TytgatS. Van PutteD. VanneromB. ClerbauxG. De LentdeckerL. FavartD. HohovJ. JaramilloA. KhalilzadehK. LeeM. MahdavikhorramiA. MalaraS. ParedesL. PétréN. PostiauL. ThomasM. Vanden BemdenC. Vander VeldeP. VanlaerM. De CoenD. DoburY. HongJ. KnolleL. LambrechtG. MestdachC. RendónA. SamalanK. SkovpenN. Van Den BosscheJ. van der LindenL. WezenbeekA. BeneckeG. BrunoC. CaputoC. DelaereI.S. DonertasA. GiammancoK. JaffelSa. JainV. LemaitreJ. LidrychP. MastrapasquaK. MondalT.T. TranS. WertzG.A. AlvesE. CoelhoC. HenselT. Menezes De OliveiraA. MoraesP. Rebello TelesM. SoeiroW.L. Aldá JúniorM. Alves Gallo PereiraM. Barroso Ferreira FilhoH. Brandao MalbouissonW. CarvalhoJ. ChinellatoE.M. Da CostaG.G. Da SilveiraD. De Jesus DamiaoS. Fonseca De SouzaJ. MartinsC. Mora HerreraK. Mota AmariloL. MundimH. NogimaA. SantoroA. SznajderM. ThielA. Vilela PereiraC.A. BernardesL. CalligarisT.R. Fernandez Perez TomeiE.M. GregoresP.G. MercadanteS.F. NovaesB. OrzariSandra S. PadulaA. AleksandrovG. AntchevR. HadjiiskaP. IaydjievM. MishevaM. ShopovaG. SultanovA. DimitrovL. LitovB. PavlovP. PetkovA. PetrovE. ShumkaS. KeshriS. ThakurT. ChengQ. GuoT. JavaidL. YuanZ. HuJ. LiuK. YiG.M. ChenH.S. ChenM. ChenF. IemmiC.H. JiangA. KapoorH. LiaoZ.-A. LiuR. SharmaJ.N. SongJ. TaoC. WangJ. WangZ. WangH. ZhangA. AgapitosY. BanA. LevinC. LiQ. LiY. MaoS.J. QianX. SunD. WangH. YangL. ZhangC. ZhouZ. YouN. LuG. BauerX. GaoD. LeggatH. OkawaY. ZhangZ. LinC. LuM. XiaoC. AvilaD.A. Barbosa TrujilloA. CabreraC. FlorezJ. FragaJ.A. Reyes VegaJ. Mejia GuisaoF. RamirezM. RodriguezJ.D. Ruiz AlvarezD. GiljanovicN. GodinovicD. LelasA. SculacM. 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BorshchD. BudkouskiV. BunichevV. ChekhovskyR. ChistovM. DanilovA. DermenevT. DimovaD. DruzhkinM. DubininL. DudkoA. ErshovG. GavrilovV. GavrilovS. GninenkoV. GolovtcovN. GolubevI. GolutvinI. GorbunovA. GribushinY. IvanovV. KachanovV. KarjavineA. KarneyeuV. KimM. KirakosyanD. KirpichnikovM. KirsanovV. KlyukhinV. KorenkovA. KozyrevN. KrasnikovA. LanevP. LevchenkoN. LychkovskayaV. MakarenkoA. MalakhovV. MatveevV. MurzinA. NikitenkoS. ObraztsovV. OreshkinV. PalichikV. PerelyginM. PerfilovS. PolikarpovV. PopovO. RadchenkoM. SavinaV. SavrinV. ShalaevS. ShmatovS. ShulhaY. SkovpenS. SlabospitskiiV. SmirnovD. SosnovV. SulimovE. TcherniaevA. TerkulovO. TeryaevI. TlisovaA. ToropinL. UvarovA. UzunianP. VolkovA. VorobyevG. VorotnikovN. VoytishinB.S. YuldashevA. ZarubinI. ZhizhinA. ZhokinCMSTop quarksExtra Higgs bosonYukawa couplingsPhysics Letters B 850 (2024). doi:10.1016/j.physletb.2024.138478journalPhysics Letters B© 2024 The Author(s). Published by Elsevier B.V. Funded by SCOAP³.Elsevier B.V.0370-2693850March 202410.1016/j.physletb.2024.138478http://dx.doi.org/10.1016/j.physletb.2024.138478doi:10.1016/j.physletb.2024.138478138478http://vtw.elsevier.com/data/voc/oa/OpenAccessStatus#Full2024-01-12T00:06:30ZSCOAP³ - Sponsoring Consortium for Open Access Publishing in Particle Physicshttp://vtw.elsevier.com/data/voc/oa/SponsorType#FundingBodyhttp://creativecommons.org/licenses/by/4.0/2024-02-02T00:00:00.000Z2024-02-09T00:00:00.000ZThis is an open access article under the CC BY license.JournalsS300.3PLB138478138478S0370-2693(24)00017-010.1016/j.physletb.2024.138478The Author(s)ExperimentsCMSdata preservation, re-use and open access policyFig. 1Representative Feynman diagram for ttq‾ (q = u, c) production through a new scalar (H) or pseudoscalar (A) Higgs boson. In this analysis, events with q = q′ are considered.Fig. 1Fig. 2The pre-fit CvsL (upper) and CvsB (lower) distributions for the selected highest pT jet. The predictions for mA = 350 GeV with A-H interference assuming mA − mH = 50 GeV for ρtu = 1.0 (solid red line) and ρtc = 1.0 (dashed red line) are also displayed. The numbers in square brackets represent the yields for each sample. The uncertainty bars on the points and the hatched bands represent the statistical uncertainties in the data and in the background predictions, respectively. Beneath each plot the ratio of data to predictions is shown. The uncertainty bars in the ratio plots include statistical uncertainties in the data and in the background predictions.Fig. 2Fig. 3Post-fit distributions of the BDT discriminants combining the categories e±e±, μ±μ±, and e±μ±, and all data-taking periods, for mA = 350 GeV with ρtu = 1.0 (upper), and ρtc = 1.0 (lower) with the A-H interference. The numbers in square brackets represent the yields for each sample. The uncertainty bars on the points represent the statistical uncertainties in the data. Beneath each plot the ratio of data to predictions is shown. The uncertainty bars in the ratio plots include statistical uncertainties in the data and the total uncertainty in the background predictions, and the hatched bands represent the total uncertainty in the background predictions.Fig. 3Fig. 4Observed and expected 95% CL upper limits on the signal strength as functions of mA for g2HDM using different coupling assumptions: ρtu = 0.1, 0.4, 1.0 (upper) and ρtc = 0.1, 0.4, 1.0 (lower) without interference, for the combination of the e±e±, μ±μ±, and e±μ± categories and all data-taking periods. The inner (green) band and the outer (yellow) band indicate the regions containing 68 and 95%, respectively, of the distribution of limits expected under the background-only hypothesis.Fig. 4Fig. 5Observed and expected 95% CL upper limits on the signal strength as functions of mA for g2HDM using different coupling assumptions: ρtu = 0.1, 0.4, 1.0 (upper) and ρtc = 0.1, 0.4, 1.0 (lower) with A-H interference assuming mA − mH = 50 GeV, for the combination of the e±e±, μ±μ±, and e±μ± categories and all data-taking periods. The inner (green) band and the outer (yellow) band indicate the regions containing 68 and 95%, respectively, of the distribution of limits expected under the background-only hypothesis.Fig. 5Fig. 6Observed 95% CL upper limit on the signal strength as a function of mA and ρtu (upper) and ρtc (lower) for g2HDM without the A-H interference, for the combination of the e±e±, μ±μ±, and e±μ± categories. The color axis represents the observed upper limit on the signal strength. Expected (dashed lines) and observed (solid lines) exclusion contours are also shown.Fig. 6Fig. 7Observed 95% CL upper limit on the signal strength as a function of mA and ρtu (upper) and ρtc (lower) for g2HDM signal model with the A-H interference, for the combination of the e±e±, μ±μ±, and e±μ± categories. The color axis represents the observed upper limit on the signal strength. Expected (dashed lines) and observed (solid lines) exclusion contours are also shown.Fig. 7Table 1Input variables of the BDT. Jets and leptons are ordered by pT.Table 1Input variables of the BDTCvsL(ja)a = 1,2,3Charm- vs light-quark jet identification variableCvsB(ja)a = 1,2,3Charm- vs bottom-quark jet identification variableΔR(ja,jb)1 ≤ a < b ≤ 3Angular separation between jetsm(ja,jb)1 ≤ a < b ≤ 3Invariant mass of jet pairsΔR(ja,lb)a = 1,2,3; b = 1,2Angular separation between jet and leptonm(ja,lb)a = 1,2,3; b = 1,2Invariant mass of jet-lepton pairspT(ℓa)a = 1,2Transverse momentum of leptonsm(ℓ1,ℓ2,ja)a = 1,2,3Invariant mass of the two leptons plus the highest pT jetm(ℓ1,ℓ2)Invariant mass of the two leptonsHTScalar pT sum of the jetspTmissMissing transverse momentumTable 2Summary of systematic uncertainties for ρtc = 0.4 and mA = 350 GeV with A-H interference assuming mA − mH = 50 GeV. The first column indicates the source of uncertainty. The second column specifies whether the shape of the fit discriminant is affected by the nuisance parameter (✓) or not (dash). The impact in percent of these nuisance parameters on the pre-fit expected event yields is displayed in the third column. This column is subdivided into three event categories representing the analysis channels. The percentage impacts are given as a range of values representing the minimum and maximum differences obtained in the different bins of the BDT distribution through the four data-taking periods. The numbers for the normalization component of the nonprompt lepton background represent the uncertainties used for each data-taking period. Whether or not a nuisance parameter is taken correlated across years and categories is specified in the last two columns. The luminosity and jet flavor identification nuisances are only partially correlated across years.Table 2Uncertainty sourceShapeCategoryCorrelated acrosse±e±μ±μ±e±μ±YearsCategoriesExperimentalLuminosity—1.2–2.51.2–2.51.2–2.5✓✓Pileup✓<0.1–2.8<0.1–1.8<0.1–2.3✓✓Trigger efficiency✓0.4–2.60.2–1.10.3–1.2——L1 trigger inefficiency✓0.1–0.80.1–0.30.1–0.4✓✓Lepton identification✓0.1–1.7<0.1–0.4<0.1–0.6—✓Lepton energy scale✓—<0.1–0.2<0.1–0.2—✓Charge misid.✓1.2–13.1————Jet energy scale✓<0.1–4.5<0.1–1.7<0.1–1.5✓✓Jet energy resolution✓<0.1–2.6<0.1–1.8<0.1–1.6—✓Unclustered energy✓<0.1–2.6<0.1–0.5<0.1–0.8—✓Jet flavor identification✓<0.1–12.1<0.1–8.8<0.1–11.6✓✓Nonprompt lepton BGstatistical component✓<0.1–27.21.9–16.23.0–13.2—✓Nonprompt lepton BG—27,15,11,1027,15,11,1027,15,11,10—✓TheoreticalSignal QCD scales✓10.3–10.510.0–10.29.9–10.0✓✓Signal PDF✓0.70.6–0.70.5–0.6✓✓Signal parton shower✓3.6–4.34.0–4.36.3–7.3✓✓tt‾—6.16.16.1✓✓VV—4.54.54.5✓✓VBS—10.410.410.4✓✓tt‾H—7.87.87.8✓✓tt‾W—10.710.710.7✓✓Other backgrounds—5.45.45.4✓✓Table 3Observed (expected) lower limits on mA at 95% CL. For the scenario without interference, the limits on mH and mA are the same.Table 3Observed (expected) mass limit [GeV]withoutwithwithinterferenceinterferenceinterferencemA or mHmAmHρtu0.4920 (920)1000 (1000)950 (950)1.01000 (1000)1000 (1000)950 (950)ρtc0.4no limit340 (370)290 (320)1.0770 (680)810 (670)760 (620)LetterSearch for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at s=13TeVThe CMS Collaboration⋆A.HayrapetyanA.Tumasyan1Yerevan Physics Institute, Yerevan, ArmeniaYerevan Physics InstituteYerevanArmeniaYerevan Physics Institute, Yerevan, Armenia1Also at Yerevan State University, Yerevan, Armenia.W.AdamJ.W.AndrejkovicT.BergauerS.ChatterjeeK.DamanakisM.DragicevicP.S.HussainM.Jeitler2N.KrammerA.LiD.LikoI.MikulecJ.Schieck2R.SchöfbeckD.SchwarzM.SonawaneS.TemplW.WaltenbergerC.-E.Wulz2Institut für Hochenergiephysik, Vienna, AustriaInstitut für HochenergiephysikViennaAustriaInstitut für Hochenergiephysik, Vienna, Austria2Also at TU Wien, Vienna, Austria.M.R.Darwish3T.JanssenP.Van MechelenUniversiteit Antwerpen, Antwerpen, BelgiumUniversiteit AntwerpenAntwerpenBelgiumUniversiteit Antwerpen, Antwerpen, Belgium3Also at Institute of Basic and Applied Sciences, Faculty of Engineering, Arab Academy for Science, Technology and Maritime Transport, Alexandria, Egypt.E.S.BolsJ.D'HondtS.DansanaA.De MoorM.DelcourtH.El FahamS.LowetteI.MakarenkoD.MüllerA.R.SahasransuS.TavernierM.Tytgat4S.Van PutteD.VanneromVrije Universiteit Brussel, Brussel, BelgiumVrije Universiteit BrusselBrusselBelgiumVrije Universiteit Brussel, Brussel, Belgium4Also at Ghent University, Ghent, Belgium.B.ClerbauxG.De LentdeckerL.FavartD.HohovJ.JaramilloA.KhalilzadehK.LeeM.MahdavikhorramiA.MalaraS.ParedesL.PétréN.PostiauL.ThomasM.Vanden BemdenC.Vander VeldeP.VanlaerUniversité Libre de Bruxelles, Bruxelles, BelgiumUniversité Libre de BruxellesBruxellesBelgiumUniversité Libre de Bruxelles, Bruxelles, BelgiumM.De CoenD.DoburY.HongJ.KnolleL.LambrechtG.MestdachC.RendónA.SamalanK.SkovpenN.Van Den BosscheJ.van der LindenL.WezenbeekGhent University, Ghent, BelgiumGhent UniversityGhentBelgiumGhent University, Ghent, BelgiumA.BeneckeG.BrunoC.CaputoC.DelaereI.S.DonertasA.GiammancoK.JaffelSa.JainV.LemaitreJ.LidrychP.MastrapasquaK.MondalT.T.TranS.WertzUniversité Catholique de Louvain, Louvain-la-Neuve, BelgiumUniversité Catholique de LouvainLouvain-la-NeuveBelgiumUniversité Catholique de Louvain, Louvain-la-Neuve, BelgiumG.A.AlvesE.CoelhoC.HenselT.Menezes De OliveiraA.MoraesP.Rebello TelesM.SoeiroCentro Brasileiro de Pesquisas Fisicas, Rio de Janeiro, BrazilCentro Brasileiro de Pesquisas FisicasRio de JaneiroBrazilCentro Brasileiro de Pesquisas Fisicas, Rio de Janeiro, BrazilW.L.Aldá JúniorM.Alves Gallo PereiraM.Barroso Ferreira FilhoH.Brandao MalbouissonW.CarvalhoJ.Chinellato5E.M.Da CostaG.G.Da Silveira6D.De Jesus DamiaoS.Fonseca De SouzaJ.Martins7C.Mora HerreraK.Mota AmariloL.MundimH.NogimaA.SantoroA.SznajderM.ThielA.Vilela PereiraUniversidade do Estado do Rio de Janeiro, Rio de Janeiro, BrazilUniversidade do Estado do Rio de JaneiroRio de JaneiroBrazilUniversidade do Estado do Rio de Janeiro, Rio de Janeiro, Brazil5Also at Universidade Estadual de Campinas, Campinas, Brazil.6Also at Federal University of Rio Grande do Sul, Porto Alegre, Brazil.7Also at UFMS, Nova Andradina, Brazil.C.A.Bernardes6L.CalligarisT.R.Fernandez Perez TomeiE.M.GregoresP.G.MercadanteS.F.NovaesB.OrzariSandra S.PadulaUniversidade Estadual Paulista, Universidade Federal do ABC, São Paulo, BrazilUniversidade Estadual PaulistaUniversidade Federal do ABCSão PauloBrazilUniversidade Estadual Paulista, Universidade Federal do ABC, São Paulo, BrazilA.AleksandrovG.AntchevR.HadjiiskaP.IaydjievM.MishevaM.ShopovaG.SultanovInstitute for Nuclear Research and Nuclear Energy, Bulgarian Academy of Sciences, Sofia, BulgariaInstitute for Nuclear Research and Nuclear EnergyBulgarian Academy of SciencesSofiaBulgariaInstitute for Nuclear Research and Nuclear Energy, Bulgarian Academy of Sciences, Sofia, BulgariaA.DimitrovL.LitovB.PavlovP.PetkovA.PetrovE.ShumkaUniversity of Sofia, Sofia, BulgariaUniversity of SofiaSofiaBulgariaUniversity of Sofia, Sofia, BulgariaS.KeshriS.ThakurInstituto De Alta Investigación, Universidad de Tarapacá, Casilla 7 D, Arica, ChileInstituto De Alta InvestigaciónUniversidad de TarapacáCasilla 7 DAricaChileInstituto De Alta Investigación, Universidad de Tarapacá, Casilla 7 D, Arica, ChileT.ChengQ.GuoT.JavaidL.YuanBeihang University, Beijing, ChinaBeihang UniversityBeijingChinaBeihang University, Beijing, ChinaZ.HuJ.LiuK.Yi89Department of Physics, Tsinghua University, Beijing, ChinaDepartment of PhysicsTsinghua UniversityBeijingChinaDepartment of Physics, Tsinghua University, Beijing, China8Also at Nanjing Normal University, Nanjing, China.9Now at The University of Iowa, Iowa City, Iowa, USA.G.M.Chen10H.S.Chen10M.Chen10F.IemmiC.H.JiangA.Kapoor11H.LiaoZ.-A.Liu12R.Sharma13J.N.Song12J.TaoC.Wang10J.WangZ.Wang10H.ZhangInstitute of High Energy Physics, Beijing, ChinaInstitute of High Energy PhysicsBeijingChinaInstitute of High Energy Physics, Beijing, China10Also at University of Chinese Academy of Sciences, Beijing, China.11Also at China Center of Advanced Science and Technology, Beijing, China.12Also at University of Chinese Academy of Sciences, Beijing, China.13Also at China Spallation Neutron Source, Guangdong, China.A.AgapitosY.BanA.LevinC.LiQ.LiY.MaoS.J.QianX.SunD.WangH.YangL.ZhangC.ZhouState Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, ChinaState Key Laboratory of Nuclear Physics and TechnologyPeking UniversityBeijingChinaState Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, ChinaZ.YouSun Yat-Sen University, Guangzhou, ChinaSun Yat-Sen UniversityGuangzhouChinaSun Yat-Sen University, Guangzhou, ChinaN.LuUniversity of Science and Technology of China, Hefei, ChinaUniversity of Science and Technology of ChinaHefeiChinaUniversity of Science and Technology of China, Hefei, ChinaG.Bauer14Nanjing Normal University, Nanjing, ChinaNanjing Normal UniversityNanjingChinaNanjing Normal University, Nanjing, China14Now at Henan Normal University, Xinxiang, China.X.Gao15D.LeggatH.OkawaY.ZhangInstitute of Modern Physics and Key Laboratory of Nuclear Physics and Ion-beam Application (MOE) - Fudan University, Shanghai, ChinaInstitute of Modern PhysicsKey Laboratory of Nuclear PhysicsIon-beam Application (MOE)Fudan UniversityShanghaiChinaInstitute of Modern Physics and Key Laboratory of Nuclear Physics and Ion-beam Application (MOE) - Fudan University, Shanghai, China15Also at Université Libre de Bruxelles, Bruxelles, Belgium.Z.LinC.LuM.XiaoZhejiang University, Hangzhou, Zhejiang, ChinaZhejiang UniversityHangzhouZhejiangChinaZhejiang University, Hangzhou, Zhejiang, ChinaC.AvilaD.A.Barbosa TrujilloA.CabreraC.FlorezJ.FragaJ.A.Reyes VegaUniversidad de Los Andes, Bogota, ColombiaUniversidad de Los AndesBogotaColombiaUniversidad de Los Andes, Bogota, ColombiaJ.Mejia GuisaoF.RamirezM.RodriguezJ.D.Ruiz AlvarezUniversidad de Antioquia, Medellin, ColombiaUniversidad de AntioquiaMedellinColombiaUniversidad de Antioquia, Medellin, ColombiaD.GiljanovicN.GodinovicD.LelasA.SculacUniversity of Split, Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, Split, CroatiaUniversity of SplitFaculty of Electrical Engineering, Mechanical Engineering and Naval ArchitectureSplitCroatiaUniversity of Split, Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, Split, CroatiaM.KovacT.Sculac16University of Split, Faculty of Science, Split, CroatiaUniversity of SplitFaculty of ScienceSplitCroatiaUniversity of Split, Faculty of Science, Split, Croatia16Also at University of Latvia (LU), Riga, Latvia.P.BargassaV.BrigljevicB.K.ChitrodaD.FerencekS.MishraA.Starodumov17T.SusaInstitute Rudjer Boskovic, Zagreb, CroatiaInstitute Rudjer BoskovicZagrebCroatiaInstitute Rudjer Boskovic, Zagreb, Croatia17Also at an institute or an international laboratory covered by a cooperation agreement with CERN.A.AttikisK.ChristoforouS.KonstantinouJ.MousaC.NicolaouF.PtochosP.A.RazisH.RykaczewskiH.SakaA.StepennovUniversity of Cyprus, Nicosia, CyprusUniversity of CyprusNicosiaCyprusUniversity of Cyprus, Nicosia, CyprusM.FingerM.FingerJr.A.KvetonCharles University, Prague, Czech RepublicCharles UniversityPragueCzech RepublicCharles University, Prague, Czech RepublicE.AyalaEscuela Politecnica Nacional, Quito, EcuadorEscuela Politecnica NacionalQuitoEcuadorEscuela Politecnica Nacional, Quito, EcuadorE.Carrera JarrinUniversidad San Francisco de Quito, Quito, EcuadorUniversidad San Francisco de QuitoQuitoEcuadorUniversidad San Francisco de Quito, Quito, EcuadorH.Abdalla18Y.Assran1920Academy of Scientific Research and Technology of the Arab Republic of Egypt, Egyptian Network of High Energy Physics, Cairo, EgyptAcademy of Scientific Research and Technology of the Arab Republic of EgyptEgyptian Network of High Energy PhysicsCairoEgyptAcademy of Scientific Research and Technology of the Arab Republic of Egypt, Egyptian Network of High Energy Physics, Cairo, Egypt18Also at Cairo University, Cairo, Egypt.19Also at Suez University, Suez, Egypt.20Now at British University in Egypt, Cairo, Egypt.M.A.MahmoudY.MohammedCenter for High Energy Physics (CHEP-FU), Fayoum University, El-Fayoum, EgyptCenter for High Energy Physics (CHEP-FU)Fayoum UniversityEl-FayoumEgyptCenter for High Energy Physics (CHEP-FU), Fayoum University, El-Fayoum, EgyptR.K.Dewanjee21K.EhatahtM.KadastikT.LangeS.NandanC.NielsenJ.PataM.RaidalL.TaniC.VeelkenNational Institute of Chemical Physics and Biophysics, Tallinn, EstoniaNational Institute of Chemical Physics and BiophysicsTallinnEstoniaNational Institute of Chemical Physics and Biophysics, Tallinn, Estonia21Also at Birla Institute of Technology, Mesra, Mesra, India.H.KirschenmannK.OsterbergM.VoutilainenDepartment of Physics, University of Helsinki, Helsinki, FinlandDepartment of PhysicsUniversity of HelsinkiHelsinkiFinlandDepartment of Physics, University of Helsinki, Helsinki, FinlandS.BharthuarE.BrückenF.GarciaJ.HavukainenK.T.S.KallonenR.KinnunenT.LampénK.Lassila-PeriniS.LehtiT.LindénM.LottiL.MartikainenM.MyllymäkiM.m.RantanenH.SiikonenE.TuominenJ.TuominiemiHelsinki Institute of Physics, Helsinki, FinlandHelsinki Institute of PhysicsHelsinkiFinlandHelsinki Institute of Physics, Helsinki, FinlandP.LuukkaH.PetrowT.Tuuva†Lappeenranta-Lahti University of Technology, Lappeenranta, FinlandLappeenranta-Lahti University of TechnologyLappeenrantaFinlandLappeenranta-Lahti University of Technology, Lappeenranta, Finland†Deceased.M.BesanconF.CoudercM.DejardinD.DenegriJ.L.FaureF.FerriS.GanjourP.GrasG.Hamel de MonchenaultV.LohezicJ.MalclesJ.RanderA.RosowskyM.Ö.SahinA.Savoy-Navarro22P.SimkinaM.TitovM.TornagoIRFU, CEA, Université Paris-Saclay, Gif-sur-Yvette, FranceIRFUCEAUniversité Paris-SaclayGif-sur-YvetteFranceIRFU, CEA, Université Paris-Saclay, Gif-sur-Yvette, France22Also at Purdue University, West Lafayette, Indiana, USA.C.Baldenegro BarreraF.BeaudetteA.Buchot PerraguinP.BussonA.CappatiC.CharlotF.DamasO.DavignonA.De WitG.FalmagneB.A.Fontana Santos AlvesS.GhoshA.GilbertR.Granier de CassagnacA.HakimiB.HarikrishnanL.KalipolitiG.LiuJ.MottaM.NguyenC.OchandoL.PortalesR.SalernoJ.B.SauvanY.SiroisA.TarabiniE.VernazzaA.ZabiA.ZghicheLaboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, FranceLaboratoire Leprince-RinguetCNRS/IN2P3Ecole PolytechniqueInstitut Polytechnique de ParisPalaiseauFranceLaboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, FranceJ.-L.Agram23J.AndreaD.ApparuD.BlochJ.-M.BromE.C.ChabertC.CollardS.FalkeU.GoerlachC.GrimaultR.HaeberleA.-C.Le BihanM.MeenaG.SahaM.A.SessiniP.Van HoveUniversité de Strasbourg, CNRS, IPHC UMR 7178, Strasbourg, FranceUniversité de StrasbourgCNRSIPHC UMR 7178StrasbourgFranceUniversité de Strasbourg, CNRS, IPHC UMR 7178, Strasbourg, France23Also at Université de Haute Alsace, Mulhouse, France.S.BeauceronB.BlanconG.BoudoulN.ChanonJ.ChoiD.ContardoP.DepasseC.Dozen24H.El MamouniJ.FayS.GasconM.GouzevitchC.GreenbergG.GrenierB.IlleI.B.LaktinehM.LethuillierL.MirabitoS.PerriesA.PurohitM.Vander DoncktP.VerdierJ.XiaoInstitut de Physique des 2 Infinis de Lyon (IP2I), Villeurbanne, FranceInstitut de Physique des 2 Infinis de Lyon (IP2I)VilleurbanneFranceInstitut de Physique des 2 Infinis de Lyon (IP2I ), Villeurbanne, France24Also at Department of Physics, Tsinghua University, Beijing, China.A.Khvedelidze17I.LomidzeZ.Tsamalaidze17Georgian Technical University, Tbilisi, GeorgiaGeorgian Technical UniversityTbilisiGeorgiaGeorgian Technical University, Tbilisi, GeorgiaV.BottaL.FeldK.KleinM.LipinskiD.MeuserA.PaulsN.RöwertM.TeroerdeRWTH Aachen University, I. Physikalisches Institut, Aachen, GermanyRWTH Aachen UniversityI. Physikalisches InstitutAachenGermanyRWTH Aachen University, I. Physikalisches Institut, Aachen, GermanyS.DiekmannA.DodonovaN.EichD.EliseevF.EngelkeM.ErdmannP.FackeldeyB.FischerT.HebbekerK.HoepfnerF.IvoneA.JungM.y.LeeL.MastrolorenzoF.MausolfM.MerschmeyerA.MeyerS.MukherjeeD.NollA.NovakF.NowotnyA.PozdnyakovY.RathW.RedjebF.RehmH.ReithlerU.SarkarV.SarkisoviA.SchmidtA.SharmaJ.L.SpahA.SteinF.Torres Da Silva De Araujo25L.VigilanteS.WiedenbeckS.ZaleskiRWTH Aachen University, III. Physikalisches Institut A, Aachen, GermanyRWTH Aachen UniversityIII. Physikalisches Institut AAachenGermanyRWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany25Also at The University of the State of Amazonas, Manaus, Brazil.C.DziwokG.FlüggeW.Haj Ahmad26T.KressA.NowackO.PoothA.StahlT.ZiemonsA.ZotzRWTH Aachen University, III. Physikalisches Institut B, Aachen, GermanyRWTH Aachen UniversityIII. Physikalisches Institut BAachenGermanyRWTH Aachen University, III. Physikalisches Institut B, Aachen, Germany26Also at Erzincan Binali Yildirim University, Erzincan, Turkey.H.Aarup PetersenM.Aldaya MartinJ.AlimenaS.AmorosoY.AnS.BaxterM.BayatmakouH.Becerril GonzalezO.BehnkeA.BelvedereS.BhattacharyaF.Blekman27K.Borras28D.BrunnerA.CampbellA.CardiniC.ChengF.ColombinaS.Consuegra RodríguezG.Correia SilvaM.De SilvaG.EckerlinD.EcksteinL.I.Estevez BanosO.FilatovE.Gallo27A.GeiserA.GiraldiG.GreauV.GuglielmiM.GuthoffA.HinzmannA.Jafari29L.JeppeN.Z.JomhariB.KaechM.KasemannH.KavehC.KleinwortR.KoglerM.KommD.KrückerW.LangeD.Leyva PerniaK.Lipka30W.Lohmann31R.MankelI.-A.Melzer-PellmannM.Mendizabal MorentinJ.MetwallyA.B.MeyerG.MilellaA.MussgillerL.P.NairA.NürnbergY.OtaridJ.ParkD.Pérez AdánE.RankenA.RasperezaB.Ribeiro LopesJ.RübenachA.SaggioM.Scham3228S.Schnake28P.SchützeC.Schwanenberger27D.SelivanovaM.ShchedrolosievR.E.Sosa RicardoD.StaffordF.VazzolerA.Ventura BarrosoR.WalshQ.WangY.WenK.WichmannL.Wiens28C.WissingY.YangA.Zimermmane Castro SantosDeutsches Elektronen-Synchrotron, Hamburg, GermanyDeutsches Elektronen-SynchrotronHamburgGermanyDeutsches Elektronen-Synchrotron, Hamburg, Germany27Also at University of Hamburg, Hamburg, Germany.28Also at RWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany.29Also at Isfahan University of Technology, Isfahan, Iran.30Also at Bergische University Wuppertal (BUW), Wuppertal, Germany.31Also at Brandenburg University of Technology, Cottbus, Germany.32Also at Forschungszentrum Jülich, Juelich, Germany.A.AlbrechtS.AlbrechtM.AntonelloS.BeinL.BenatoM.BonanomiP.ConnorM.EichK.El MorabitY.FischerA.FröhlichC.GarbersE.GaruttiA.GrohsjeanM.HajheidariJ.HallerH.R.JabuschG.KasieczkaP.KeicherR.KlannerW.KorcariT.KramerV.KutznerF.LabeJ.LangeA.LobanovC.MatthiesA.MehtaL.MoureauxM.MrowietzA.NigamovaY.NissanA.PaaschK.J.Pena RodriguezT.QuadfaselB.RacitiM.RiegerD.SavoiuJ.SchindlerP.SchleperM.SchröderJ.SchwandtM.SommerhalderH.StadieG.SteinbrückA.TewsM.WolfUniversity of Hamburg, Hamburg, GermanyUniversity of HamburgHamburgGermanyUniversity of Hamburg, Hamburg, GermanyS.BrommerM.BurkartE.ButzT.ChwalekA.DierlammA.DrollN.FaltermannM.GiffelsA.GottmannF.Hartmann33R.HofsaessM.HorzelaU.HusemannJ.KieselerM.KluteR.KoppenhöferJ.M.LawhornM.LinkA.LintuluotoS.MaierS.MitraM.MormileTh.MüllerM.NeukumM.OhM.PresillaG.QuastK.RabbertzB.RegneryN.ShadskiyI.ShvetsovH.J.SimonisM.Toms34N.TrevisaniR.UlrichR.F.Von CubeM.WassmerS.WielandF.WittigR.WolfS.WunschX.ZuoKarlsruher Institut fuer Technologie, Karlsruhe, GermanyKarlsruher Institut fuer TechnologieKarlsruheGermanyKarlsruher Institut fuer Technologie, Karlsruhe, Germany33Also at CERN, European Organization for Nuclear Research, Geneva, Switzerland.34Now at an institute or an international laboratory covered by a cooperation agreement with CERN.G.AnagnostouG.DaskalakisA.KyriakisA.Papadopoulos33A.StakiaInstitute of Nuclear and Particle Physics (INPP), NCSR Demokritos, Aghia Paraskevi, GreeceInstitute of Nuclear and Particle Physics (INPP)NCSR DemokritosAghia ParaskeviGreeceInstitute of Nuclear and Particle Physics (INPP), NCSR Demokritos, Aghia Paraskevi, GreeceP.KontaxakisG.MelachroinosA.PanagiotouI.PapavergouI.ParaskevasN.SaoulidouK.TheofilatosE.TziaferiK.VellidisI.ZisopoulosNational and Kapodistrian University of Athens, Athens, GreeceNational and Kapodistrian University of AthensAthensGreeceNational and Kapodistrian University of Athens, Athens, GreeceG.BakasT.ChatzistavrouG.KarapostoliK.KousourisI.PapakrivopoulosE.SiamarkouG.TsipolitisA.ZacharopoulouNational Technical University of Athens, Athens, GreeceNational Technical University of AthensAthensGreeceNational Technical University of Athens, Athens, GreeceK.AdamidisI.BestintzanosI.EvangelouC.FoudasP.GianneiosC.KamtsikisP.KatsoulisP.KokkasP.G.Kosmoglou KioseoglouN.ManthosI.PapadopoulosJ.StrologasUniversity of Ioánnina, Ioánnina, GreeceUniversity of IoánninaIoánninaGreeceUniversity of Ioánnina, Ioánnina, GreeceM.Bartók35C.HajduD.Horvath3637F.SiklerV.VeszpremiHUN-REN Wigner Research Centre for Physics, Budapest, HungaryHUN-REN Wigner Research Centre for PhysicsBudapestHungaryHUN-REN Wigner Research Centre for Physics, Budapest, Hungary35Also at Institute of Physics, University of Debrecen, Debrecen, Hungary.36Also at Institute of Nuclear Research ATOMKI, Debrecen, Hungary.37Now at Universitatea Babes-Bolyai - Facultatea de Fizica, Cluj-Napoca, Romania.M.CsanádK.FarkasM.M.A.Gadallah38Á.KadlecsikP.MajorK.MandalG.PásztorA.J.Rádl39G.I.VeresMTA-ELTE Lendület CMS Particle and Nuclear Physics Group, Eötvös Loránd University, Budapest, HungaryMTA-ELTE Lendület CMS Particle and Nuclear Physics GroupEötvös Loránd UniversityBudapestHungaryMTA-ELTE Lendület CMS Particle and Nuclear Physics Group, Eötvös Loránd University, Budapest, Hungary38Also at Physics Department, Faculty of Science, Assiut University, Assiut, Egypt.39Also at HUN-REN Wigner Research Centre for Physics, Budapest, Hungary.P.RaicsB.UjvariG.ZiliziFaculty of Informatics, University of Debrecen, Debrecen, HungaryFaculty of InformaticsUniversity of DebrecenDebrecenHungaryFaculty of Informatics, University of Debrecen, Debrecen, HungaryG.BenczeS.CzellarJ.Karancsi35J.MolnarZ.SzillasiInstitute of Nuclear Research ATOMKI, Debrecen, HungaryInstitute of Nuclear Research ATOMKIDebrecenHungaryInstitute of Nuclear Research ATOMKI, Debrecen, HungaryT.Csorgo39F.Nemes39T.NovakKaroly Robert Campus, MATE Institute of Technology, Gyongyos, HungaryMATE Institute of TechnologyKaroly Robert CampusGyongyosHungaryKaroly Robert Campus, MATE Institute of Technology, Gyongyos, HungaryJ.BabbarS.BansalS.B.BeriV.BhatnagarG.ChaudharyS.ChauhanN.Dhingra40A.KaurA.KaurH.KaurM.KaurS.KumarK.SandeepT.SheokandJ.B.SinghA.SinglaPanjab University, Chandigarh, IndiaPanjab UniversityChandigarhIndiaPanjab University, Chandigarh, India40Also at Punjab Agricultural University, Ludhiana, India.A.AhmedA.BhardwajA.ChhetriB.C.ChoudharyA.KumarA.KumarM.NaimuddinK.RanjanS.SaumyaUniversity of Delhi, Delhi, IndiaUniversity of DelhiDelhiIndiaUniversity of Delhi, Delhi, IndiaS.BaradiaS.Barman41S.BhattacharyaS.DuttaS.DuttaP.PalitS.SarkarSaha Institute of Nuclear Physics, HBNI, Kolkata, IndiaSaha Institute of Nuclear PhysicsHBNIKolkataIndiaSaha Institute of Nuclear Physics, HBNI, Kolkata, India41Also at University of Visva-Bharati, Santiniketan, India.M.M.AmeenP.K.BeheraS.C.BeheraS.ChatterjeeP.JanaP.KalbhorJ.R.Komaragiri42D.Kumar42L.Panwar42P.R.PujahariN.R.SahaA.SharmaA.K.SikdarS.VermaIndian Institute of Technology Madras, Madras, IndiaIndian Institute of Technology MadrasMadrasIndiaIndian Institute of Technology Madras, Madras, India42Also at Indian Institute of Science (IISc), Bangalore, India.S.DugadM.KumarG.B.MohantyP.SuryadevaraTata Institute of Fundamental Research-A, Mumbai, IndiaTata Institute of Fundamental Research-AMumbaiIndiaTata Institute of Fundamental Research-A, Mumbai, IndiaA.BalaS.BanerjeeR.M.ChatterjeeM.GuchaitSh.JainS.KarmakarS.KumarG.MajumderK.MazumdarS.ParoliaA.ThachayathTata Institute of Fundamental Research-B, Mumbai, IndiaTata Institute of Fundamental Research-BMumbaiIndiaTata Institute of Fundamental Research-B, Mumbai, IndiaS.Bahinipati43A.K.DasC.KarD.Maity44P.MalT.MishraV.K.Muraleedharan Nair Bindhu44K.Naskar44A.Nayak44P.SadangiP.SahaS.K.SwainS.Varghese44D.Vats44National Institute of Science Education and Research, An OCC of Homi Bhabha National Institute, Bhubaneswar, Odisha, IndiaNational Institute of Science Education and ResearchAn OCC of Homi Bhabha National InstituteBhubaneswarOdishaIndiaNational Institute of Science Education and Research, An OCC of Homi Bhabha National Institute, Bhubaneswar, Odisha, India43Also at IIT Bhubaneswar, Bhubaneswar, India.44Also at Institute of Physics, Bhubaneswar, India.S.Acharya45A.AlpanaS.DubeB.Gomber45B.KansalA.LahaB.Sahu45S.SharmaIndian Institute of Science Education and Research (IISER), Pune, IndiaIndian Institute of Science Education and Research (IISER)PuneIndiaIndian Institute of Science Education and Research (IISER), Pune, India45Also at University of Hyderabad, Hyderabad, India.H.Bakhshiansohi46E.Khazaie47M.Zeinali48Isfahan University of Technology, Isfahan, IranIsfahan University of TechnologyIsfahanIranIsfahan University of Technology, Isfahan, Iran46Also at Deutsches Elektronen-Synchrotron, Hamburg, Germany.47Also at Department of Physics, Isfahan University of Technology, Isfahan, Iran.48Also at Sharif University of Technology, Tehran, Iran.S.Chenarani49S.M.EtesamiM.KhakzadM.Mohammadi NajafabadiInstitute for Research in Fundamental Sciences (IPM), Tehran, IranInstitute for Research in Fundamental Sciences (IPM)TehranIranInstitute for Research in Fundamental Sciences (IPM), Tehran, Iran49Also at Department of Physics, University of Science and Technology of Mazandaran, Behshahr, Iran.M.GrunewaldUniversity College Dublin, Dublin, IrelandUniversity College DublinDublinIrelandUniversity College Dublin, Dublin, IrelandM.AbbresciaabR.Alyac50A.ColaleoabD.CreanzaacB.D'AnziabN.De FilippisacM.De PalmaabA.Di FlorioacW.Elmetenaweeab50L.FioreaG.IaselliacM.LoukaabG.MaggiacM.MaggiaI.MargjekaabV.MastrapasquaabS.MyabS.NuzzoabA.PellecchiaabA.PompiliabG.PuglieseacR.RadognaaG.Ramirez-SanchezacD.RamosaA.RanieriaL.SilvestrisaF.M.SimoneabÜ.SözbiliraA.StamerraaR.VendittiaP.VerwilligenaA.ZazaabaINFN Sezione di Bari, Bari, ItalyINFN Sezione di BariBariItalyINFN Sezione di Bari, Bari, ItalybUniversità di Bari, Bari, ItalyUniversità di BariBariItalyUniversità di Bari, Bari, ItalycPolitecnico di Bari, Bari, ItalyPolitecnico di BariBariItalyPolitecnico di Bari, Bari, Italy50Also at Helwan University, Cairo, Egypt.G.AbbiendiaC.BattilanaabD.BonacorsiabL.BorgonoviaR.CampaniniabP.CapiluppiabA.CastroabF.R.CavalloaM.CuffianiabG.M.DallavalleaT.DiotaleviabF.FabbriaA.FanfaniabD.FasanellaabP.GiacomelliaL.GiommiabC.GrandiaL.GuiducciabS.Lo Meoa51L.LunertiabS.MarcelliniaG.MasettiaF.L.NavarriaabA.PerrottaaF.PrimaveraabA.M.RossiabG.P.SiroliabaINFN Sezione di Bologna, Bologna, ItalyINFN Sezione di BolognaBolognaItalyINFN Sezione di Bologna, Bologna, ItalybUniversità di Bologna, Bologna, ItalyUniversità di BolognaBolognaItalyUniversità di Bologna, Bologna, Italy51Also at Italian National Agency for New Technologies, Energy and Sustainable Economic Development, Bologna, Italy.S.Costaab52A.Di MattiaaR.PotenzaabA.Tricomiab52C.TuveabaINFN Sezione di Catania, Catania, ItalyINFN Sezione di CataniaCataniaItalyINFN Sezione di Catania, Catania, ItalybUniversità di Catania, Catania, ItalyUniversità di CataniaCataniaItalyUniversità di Catania, Catania, Italy52Also at Centro Siciliano di Fisica Nucleare e di Struttura Della Materia, Catania, Italy.P.AssiourasaG.BarbagliaG.BardelliabB.CamaianiabA.CasseseaR.CeccarelliaV.CiulliabC.CivininiaR.D'AlessandroabE.FocardiabT.KelloaG.LatinoabP.LenziabM.LizzoaM.MeschiniaS.PaolettiaA.PapanastassiouabG.SguazzoniaL.VilianiaaINFN Sezione di Firenze, Firenze, ItalyINFN Sezione di FirenzeFirenzeItalyINFN Sezione di Firenze, Firenze, ItalybUniversità di Firenze, Firenze, ItalyUniversità di FirenzeFirenzeItalyUniversità di Firenze, Firenze, ItalyL.BenussiS.BiancoS.Meola53D.PiccoloINFN Laboratori Nazionali di Frascati, Frascati, ItalyINFN Laboratori Nazionali di FrascatiFrascatiItalyINFN Laboratori Nazionali di Frascati, Frascati, Italy53Also at Università degli Studi Guglielmo Marconi, Roma, Italy.P.ChatagnonaF.FerroaE.RobuttiaS.TosiabaINFN Sezione di Genova, Genova, ItalyINFN Sezione di GenovaGenovaItalyINFN Sezione di Genova, Genova, ItalybUniversità di Genova, Genova, ItalyUniversità di GenovaGenovaItalyUniversità di Genova, Genova, ItalyA.BenagliaaG.BoldriniabF.BrivioaF.CetorelliaF.De GuioabM.E.DinardoabP.DiniaS.GennaiaR.GerosaabA.GhezziabP.GovoniabL.GuzziaM.T.LucchiniabM.MalbertiaS.MalvezziaA.MassironiaD.MenasceaL.MoroniaM.PaganoniabD.PedriniaB.S.PinoliniaS.RagazziabT.Tabarelli de FatisabD.ZuoloaaINFN Sezione di Milano-Bicocca, Milano, ItalyINFN Sezione di Milano-BicoccaMilanoItalyINFN Sezione di Milano-Bicocca, Milano, ItalybUniversità di Milano-Bicocca, Milano, ItalyUniversità di Milano-BicoccaMilanoItalyUniversità di Milano-Bicocca, Milano, ItalyS.BuontempoaA.CagnottaabF.CarnevaliabN.CavalloacA.De IorioabF.FabozziacA.O.M.IorioabL.Listaab54P.Paoluccia33B.RossiaC.SciaccaabaINFN Sezione di Napoli, Napoli, ItalyINFN Sezione di NapoliNapoliItalyINFN Sezione di Napoli, Napoli, ItalybUniversità di Napoli ‘Federico II’, Napoli, ItalyUniversità di Napoli ‘Federico II’NapoliItalyUniversità di Napoli ‘Federico II’, Napoli, ItalycUniversità della Basilicata, Potenza, ItalyUniversità della BasilicataPotenzaItalyUniversità della Basilicata, Potenza, ItalydUniversità G. Marconi, Roma, ItalyUniversità G. MarconiRomaItalyUniversità G. Marconi, Roma, Italy54Also at Scuola Superiore Meridionale, Università di Napoli ‘Federico II’, Napoli, Italy.R.ArdinoaP.AzziaN.Bacchettaa55D.BiselloabP.BortignonaA.BragagnoloabR.CarlinabP.ChecchiaaT.DorigoaF.FanzagoaU.GaspariniabF.GonellaaE.LusianiaM.MargoniabM.MiglioriniabJ.PazziniabP.RoncheseabR.RossinabF.SimonettoabG.StrongaM.TosiabA.TriossiabS.VenturaaH.YararabM.ZanettiabP.ZottoabA.ZucchettaabG.ZumerleabaINFN Sezione di Padova, Padova, ItalyINFN Sezione di PadovaPadovaItalyINFN Sezione di Padova, Padova, ItalybUniversità di Padova, Padova, ItalyUniversità di PadovaPadovaItalyUniversità di Padova, Padova, ItalycUniversità di Trento, Trento, ItalyUniversità di TrentoTrentoItalyUniversità di Trento, Trento, Italy55Also at Fermi National Accelerator Laboratory, Batavia, Illinois, USA.S.Abu Zeida56C.AimèabA.BraghieriaS.CalzaferriaD.FiorinaaP.MontagnaabV.ReaC.RiccardiabP.SalviniaI.VaiabP.VituloabaINFN Sezione di Pavia, Pavia, ItalyINFN Sezione di PaviaPaviaItalyINFN Sezione di Pavia, Pavia, ItalybUniversità di Pavia, Pavia, ItalyUniversità di PaviaPaviaItalyUniversità di Pavia, Pavia, Italy56Also at Ain Shams University, Cairo, Egypt.S.AjmalabP.Asenova57G.M.BileiaD.CiangottiniabL.FanòabM.MagheriniabG.MantovaniabV.MarianiabM.MenichelliaF.Moscatellia57A.RossiabA.SantocchiaabD.SpigaaT.TedeschiabaINFN Sezione di Perugia, Perugia, ItalyINFN Sezione di PerugiaPerugiaItalyINFN Sezione di Perugia, Perugia, ItalybUniversità di Perugia, Perugia, ItalyUniversità di PerugiaPerugiaItalyUniversità di Perugia, Perugia, Italy57Also at Consiglio Nazionale delle Ricerche - Istituto Officina dei Materiali, Perugia, Italy.P.AzzurriaG.BagliesiaR.BhattacharyaaL.BianchiniabT.BoccaliaE.BossiniaD.BruschiniacR.CastaldiaM.A.CiocciabM.CiprianiabV.D'AmanteadR.Dell'OrsoaS.DonatoaA.GiassiaF.LigabueacD.Matos FigueiredoaA.MessineoabM.MusichabF.PallaaA.RizziabG.RolandiacS.Roy ChowdhuryaT.SarkaraA.ScribanoaP.SpagnoloaR.TenchiniaG.TonelliabN.TuriniadA.VenturiaP.G.VerdiniaaINFN Sezione di Pisa, Pisa, ItalyINFN Sezione di PisaPisaItalyINFN Sezione di Pisa, Pisa, ItalybUniversità di Pisa, Pisa, ItalyUniversità di PisaPisaItalyUniversità di Pisa, Pisa, ItalycScuola Normale Superiore di Pisa, Pisa, ItalyScuola Normale Superiore di PisaPisaItalyScuola Normale Superiore di Pisa, Pisa, ItalydUniversità di Siena, Siena, ItalyUniversità di SienaSienaItalyUniversità di Siena, Siena, ItalyP.BarriaaM.CampanaabF.CavallariaL.Cunqueiro MendezabD.Del ReabE.Di MarcoaM.DiemozaF.ErricoabE.LongoabP.MeridianiaJ.MijuskovicabG.OrgantiniabF.PandolfiaR.ParamattiabC.QuarantaabS.RahatlouabC.RovelliaF.SantanastasioabL.SoffiaaINFN Sezione di Roma, Roma, ItalyINFN Sezione di RomaRomaItalyINFN Sezione di Roma, Roma, ItalybSapienza Università di Roma, Roma, ItalySapienza Università di RomaRomaItalySapienza Università di Roma, Roma, ItalyN.AmapaneabR.ArcidiaconoacS.ArgiroabM.ArneodoacN.BartosikaR.BellanabA.BelloraabC.BiinoaN.CartigliaaM.CostaabR.CovarelliabN.DemariaaL.FincoaM.GrippoabB.KianiabF.LeggeraF.LuongoabC.MariottiaS.MaselliaA.MeccaabE.MiglioreabM.MontenoaR.MulargiaaM.M.ObertinoabG.OrtonaaL.PacherabN.PastroneaM.PelliccioniaM.RuspaacF.SivieroabV.SolaabA.SolanoabA.StaianoaC.TarriconeabD.TrocinoaG.UmoretabE.VlasovabaINFN Sezione di Torino, Torino, ItalyINFN Sezione di TorinoTorinoItalyINFN Sezione di Torino, Torino, ItalybUniversità di Torino, Torino, ItalyUniversità di TorinoTorinoItalyUniversità di Torino, Torino, ItalycUniversità del Piemonte Orientale, Novara, ItalyUniversità del Piemonte OrientaleNovaraItalyUniversità del Piemonte Orientale, Novara, ItalyS.BelforteaV.CandeliseabM.CasarsaaF.CossuttiaK.De LeoabG.Della RiccaabaINFN Sezione di Trieste, Trieste, ItalyINFN Sezione di TriesteTriesteItalyINFN Sezione di Trieste, Trieste, ItalybUniversità di Trieste, Trieste, ItalyUniversità di TriesteTriesteItalyUniversità di Trieste, Trieste, ItalyS.DograJ.HongC.HuhB.KimD.H.KimJ.KimH.LeeS.W.LeeC.S.MoonY.D.OhM.S.RyuS.SekmenY.C.YangKyungpook National University, Daegu, KoreaKyungpook National UniversityDaeguKoreaKyungpook National University, Daegu, KoreaM.S.KimDepartment of Mathematics and Physics - GWNU, Gangneung, KoreaDepartment of Mathematics and Physics - GWNUGangneungKoreaDepartment of Mathematics and Physics - GWNU, Gangneung, KoreaG.BakP.GwakH.KimD.H.MoonChonnam National University, Institute for Universe and Elementary Particles, Kwangju, KoreaChonnam National UniversityInstitute for Universe and Elementary ParticlesKwangjuKoreaChonnam National University, Institute for Universe and Elementary Particles, Kwangju, KoreaE.AsilarD.KimT.J.KimJ.A.MerlinHanyang University, Seoul, KoreaHanyang UniversitySeoulKoreaHanyang University, Seoul, KoreaS.ChoiS.HanB.HongK.LeeK.S.LeeS.LeeJ.ParkS.K.ParkJ.YooKorea University, Seoul, KoreaKorea UniversitySeoulKoreaKorea University, Seoul, KoreaJ.GohS.YangKyung Hee University, Department of Physics, Seoul, KoreaKyung Hee UniversityDepartment of PhysicsSeoulKoreaKyung Hee University, Department of Physics, Seoul, KoreaH.S.KimY.KimS.LeeSejong University, Seoul, KoreaSejong UniversitySeoulKoreaSejong University, Seoul, KoreaJ.AlmondJ.H.BhyunJ.ChoiW.JunJ.KimJ.S.KimS.KoH.KwonH.LeeJ.LeeJ.LeeB.H.OhS.B.OhH.SeoU.K.YangI.YoonSeoul National University, Seoul, KoreaSeoul National UniversitySeoulKoreaSeoul National University, Seoul, KoreaW.JangD.Y.KangY.KangS.KimB.KoJ.S.H.LeeY.LeeI.C.ParkY.RohI.J.WatsonUniversity of Seoul, Seoul, KoreaUniversity of SeoulSeoulKoreaUniversity of Seoul, Seoul, KoreaS.HaH.D.YooYonsei University, Department of Physics, Seoul, KoreaYonsei UniversityDepartment of PhysicsSeoulKoreaYonsei University, Department of Physics, Seoul, KoreaM.ChoiM.R.KimH.LeeY.LeeI.YuSungkyunkwan University, Suwon, KoreaSungkyunkwan UniversitySuwonKoreaSungkyunkwan University, Suwon, KoreaT.BeyrouthyY.MaghrbiCollege of Engineering and Technology, American University of the Middle East (AUM), Dasman, KuwaitCollege of Engineering and TechnologyAmerican University of the Middle East (AUM)DasmanKuwaitCollege of Engineering and Technology, American University of the Middle East (AUM), Dasman, KuwaitK.DreimanisA.GaileG.PikursA.PotrebkoM.SeidelV.Veckalns58Riga Technical University, Riga, LatviaRiga Technical UniversityRigaLatviaRiga Technical University, Riga, Latvia58Also at Riga Technical University, Riga, Latvia.N.R.StrautnieksUniversity of Latvia (LU), Riga, LatviaUniversity of Latvia (LU)RigaLatviaUniversity of Latvia (LU), Riga, LatviaM.AmbrozasA.JuodagalvisA.RinkeviciusG.TamulaitisVilnius University, Vilnius, LithuaniaVilnius UniversityVilniusLithuaniaVilnius University, Vilnius, LithuaniaN.Bin NorjoharuddeenI.Yusuff59Z.ZolkapliNational Centre for Particle Physics, Universiti Malaya, Kuala Lumpur, MalaysiaNational Centre for Particle PhysicsUniversiti MalayaKuala LumpurMalaysiaNational Centre for Particle Physics, Universiti Malaya, Kuala Lumpur, Malaysia59Also at Department of Applied Physics, Faculty of Science and Technology, Universiti Kebangsaan Malaysia, Bangi, Malaysia.J.F.BenitezA.Castaneda HernandezH.A.Encinas AcostaL.G.Gallegos MaríñezM.León CoelloJ.A.Murillo QuijadaA.SehrawatL.Valencia PalomoUniversidad de Sonora (UNISON), Hermosillo, MexicoUniversidad de Sonora (UNISON)HermosilloMexicoUniversidad de Sonora (UNISON), Hermosillo, MexicoG.AyalaH.Castilla-ValdezE.De La Cruz-BureloI.Heredia-De La Cruz60R.Lopez-FernandezC.A.Mondragon HerreraA.Sánchez HernándezCentro de Investigacion y de Estudios Avanzados del IPN, Mexico City, MexicoCentro de Investigacion y de Estudios Avanzados del IPNMexico CityMexicoCentro de Investigacion y de Estudios Avanzados del IPN, Mexico City, Mexico60Also at Consejo Nacional de Ciencia y Tecnología, Mexico City, Mexico.C.Oropeza BarreraM.Ramírez GarcíaUniversidad Iberoamericana, Mexico City, MexicoUniversidad IberoamericanaMexico CityMexicoUniversidad Iberoamericana, Mexico City, MexicoI.BautistaI.PedrazaH.A.Salazar IbarguenC.Uribe EstradaBenemerita Universidad Autonoma de Puebla, Puebla, MexicoBenemerita Universidad Autonoma de PueblaPueblaMexicoBenemerita Universidad Autonoma de Puebla, Puebla, MexicoI.BubanjaN.RaicevicUniversity of Montenegro, Podgorica, MontenegroUniversity of MontenegroPodgoricaMontenegroUniversity of Montenegro, Podgorica, MontenegroP.H.ButlerUniversity of Canterbury, Christchurch, New ZealandUniversity of CanterburyChristchurchNew ZealandUniversity of Canterbury, Christchurch, New ZealandA.AhmadM.I.AsgharA.AwaisM.I.M.AwanH.R.HooraniW.A.KhanNational Centre for Physics, Quaid-I-Azam University, Islamabad, PakistanNational Centre for PhysicsQuaid-I-Azam UniversityIslamabadPakistanNational Centre for Physics, Quaid-I-Azam University, Islamabad, PakistanV.AvatiL.GrzankaM.MalawskiAGH University of Krakow, Faculty of Computer Science, Electronics and Telecommunications, Krakow, PolandAGH University of KrakowFaculty of Computer Science, Electronics and TelecommunicationsKrakowPolandAGH University of Krakow, Faculty of Computer Science, Electronics and Telecommunications, Krakow, PolandH.BialkowskaM.BlujB.BoimskaM.GórskiM.KazanaM.SzleperP.ZalewskiNational Centre for Nuclear Research, Swierk, PolandNational Centre for Nuclear ResearchSwierkPolandNational Centre for Nuclear Research, Swierk, PolandK.BunkowskiK.DorobaA.KalinowskiM.KoneckiJ.KrolikowskiA.MuhammadInstitute of Experimental Physics, Faculty of Physics, University of Warsaw, Warsaw, PolandInstitute of Experimental PhysicsFaculty of PhysicsUniversity of WarsawWarsawPolandInstitute of Experimental Physics, Faculty of Physics, University of Warsaw, Warsaw, PolandK.PozniakW.ZabolotnyWarsaw University of Technology, Warsaw, PolandWarsaw University of TechnologyWarsawPolandWarsaw University of Technology, Warsaw, PolandM.AraujoD.BastosC.Beirão Da Cruz E SilvaA.BolettiM.BozzoT.CamporesiG.Da MolinP.FaccioliM.GallinaroJ.HollarN.LeonardoT.NiknejadA.PetrilliM.PisanoJ.SeixasJ.VarelaJ.W.WulffLaboratório de Instrumentação e Física Experimental de Partículas, Lisboa, PortugalLaboratório de Instrumentação e Física Experimental de PartículasLisboaPortugalLaboratório de Instrumentação e Física Experimental de Partículas, Lisboa, PortugalP.AdzicP.MilenovicFaculty of Physics, University of Belgrade, Belgrade, SerbiaFaculty of PhysicsUniversity of BelgradeBelgradeSerbiaFaculty of Physics, University of Belgrade, Belgrade, SerbiaM.DordevicJ.MilosevicV.RekovicVINCA Institute of Nuclear Sciences, University of Belgrade, Belgrade, SerbiaVINCA Institute of Nuclear SciencesUniversity of BelgradeBelgradeSerbiaVINCA Institute of Nuclear Sciences, University of Belgrade, Belgrade, SerbiaM.Aguilar-BenitezJ.Alcaraz MaestreCristina F.BedoyaM.CepedaM.CerradaN.ColinoB.De La CruzA.Delgado PerisA.Escalante Del ValleD.Fernández Del ValJ.P.Fernández RamosJ.FlixM.C.FouzO.Gonzalez LopezS.Goy LopezJ.M.HernandezM.I.JosaD.MoranC.M.Morcillo PerezÁ.Navarro TobarC.Perez DengraA.Pérez-Calero YzquierdoJ.Puerta PelayoI.RedondoD.D.Redondo FerreroL.RomeroS.Sánchez NavasL.Urda GómezJ.Vazquez EscobarC.WillmottCentro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, SpainCentro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT)MadridSpainCentro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, SpainJ.F.de TrocónizUniversidad Autónoma de Madrid, Madrid, SpainUniversidad Autónoma de MadridMadridSpainUniversidad Autónoma de Madrid, Madrid, SpainB.Alvarez GonzalezJ.CuevasJ.Fernandez MenendezS.FolguerasI.Gonzalez CaballeroJ.R.González FernándezE.Palencia CortezonC.Ramón ÁlvarezV.Rodríguez BouzaA.Soto RodríguezA.TrapoteC.Vico VillalbaP.VischiaUniversidad de Oviedo, Instituto Universitario de Ciencias y Tecnologías Espaciales de Asturias (ICTEA), Oviedo, SpainUniversidad de OviedoInstituto Universitario de Ciencias y Tecnologías Espaciales de Asturias (ICTEA)OviedoSpainUniversidad de Oviedo, Instituto Universitario de Ciencias y Tecnologías Espaciales de Asturias (ICTEA), Oviedo, SpainS.BhowmikS.Blanco FernándezJ.A.Brochero CifuentesI.J.CabrilloA.CalderonJ.Duarte CampderrosM.FernandezG.GomezC.Lasaosa GarcíaC.Martinez RiveroP.Martinez Ruiz del ArbolF.MatorrasP.Matorras CuevasE.Navarrete RamosJ.Piedra GomezL.ScodellaroI.VilaJ.M.Vizan GarciaInstituto de Física de Cantabria (IFCA), CSIC-Universidad de Cantabria, Santander, SpainInstituto de Física de Cantabria (IFCA)CSIC-Universidad de CantabriaSantanderSpainInstituto de Física de Cantabria (IFCA), CSIC-Universidad de Cantabria, Santander, SpainM.K.JayanandaB.Kailasapathy61D.U.J.SonnadaraD.D.C.WickramarathnaUniversity of Colombo, Colombo, Sri LankaUniversity of ColomboColomboSri LankaUniversity of Colombo, Colombo, Sri Lanka61Also at Trincomalee Campus, Eastern University, Sri Lanka, Nilaveli, Sri Lanka.W.G.D.Dharmaratna62K.LiyanageN.PereraN.WickramageUniversity of Ruhuna, Department of Physics, Matara, Sri LankaUniversity of RuhunaDepartment of PhysicsMataraSri LankaUniversity of Ruhuna, Department of Physics, Matara, Sri Lanka62Also at Saegis Campus, Nugegoda, Sri Lanka.D.AbbaneoC.AmendolaE.AuffrayG.AuzingerJ.BaechlerD.BarneyA.Bermúdez MartínezM.BiancoB.BilinA.A.Bin AnuarA.BocciE.BrondolinC.CaillolG.CerminaraN.ChernyavskayaD.d'EnterriaA.DabrowskiA.DavidA.De RoeckM.M.DefranchisM.DeileM.DobsonF.Fallavollita63L.ForthommeG.FranzoniW.FunkS.GianiD.GigiK.GillF.GlegeL.GouskosM.HarankoJ.HegemanB.HuberV.InnocenteT.JamesP.JanotS.LaurilaP.LecoqE.LeutgebC.LourençoB.MaierL.MalgeriM.MannelliA.C.MariniM.MatthewmanF.MeijersS.MersiE.MeschiV.MilosevicF.MontiF.MoortgatM.MuldersI.NeutelingsS.OrfanelliF.PantaleoG.PetruccianiA.PfeifferM.PieriniD.PiparoH.QuD.RabadyG.Reales GutiérrezM.RovereH.SakulinS.ScarfiC.SchwickM.SelvaggiA.SharmaK.ShchelinaP.SilvaP.Sphicas64A.G.Stahl LeitonA.SteenS.SummersD.TreilleP.TropeaA.TsirouD.WalterJ.Wanczyk65J.WangS.WuchterlP.ZehetnerP.ZejdlW.D.ZeunerCERN, European Organization for Nuclear Research, Geneva, SwitzerlandCERNEuropean Organization for Nuclear ResearchGenevaSwitzerlandCERN, European Organization for Nuclear Research, Geneva, Switzerland63Also at INFN Sezione di Pavia, Università di Pavia, Pavia, Italy.64Also at National and Kapodistrian University of Athens, Athens, Greece.65Also at Ecole Polytechnique Fédérale Lausanne, Lausanne, Switzerland.T.Bevilacqua66L.Caminada66A.EbrahimiW.ErdmannR.HorisbergerQ.IngramH.C.KaestliD.KotlinskiC.LangeM.Missiroli66L.Noehte66T.RohePaul Scherrer Institut, Villigen, SwitzerlandPaul Scherrer InstitutVilligenSwitzerlandPaul Scherrer Institut, Villigen, Switzerland66Also at Universität Zürich, Zurich, Switzerland.T.K.AarrestadK.Androsov65M.BackhausA.CalandriC.CazzanigaK.DattaA.De CosaG.DissertoriM.DittmarM.DonegàF.EbleM.GalliK.GediaF.GlessgenC.GrabD.HitsW.LustermannA.-M.LyonR.A.ManzoniM.MarchegianiL.MarcheseC.Martin PerezA.Mascellani65F.Nessi-TedaldiF.PaussV.PerovicS.PigazziniM.ReichmannC.ReisselT.ReitenspiessB.RisticF.RitiD.RuiniD.A.Sanz BecerraR.SeiditaJ.Steggemann65D.ValsecchiR.WallnyETH Zurich - Institute for Particle Physics and Astrophysics (IPA), Zurich, SwitzerlandETH ZurichInstitute for Particle Physics and Astrophysics (IPA)ZurichSwitzerlandETH Zurich - Institute for Particle Physics and Astrophysics (IPA), Zurich, SwitzerlandC.Amsler67P.BärtschiC.BottaD.BrzhechkoM.F.CanelliK.CormierR.Del BurgoJ.K.HeikkiläM.HuwilerW.JinA.JofreheiB.KilminsterS.LeontsinisS.P.LiechtiA.MacchioloP.MeiringV.M.MikuniU.MolinattiA.ReimersP.RobmannS.Sanchez CruzK.SchweigerM.SengerY.TakahashiR.TramontanoUniversität Zürich, Zurich, SwitzerlandUniversität ZürichZurichSwitzerlandUniversität Zürich, Zurich, Switzerland67Also at Stefan Meyer Institute for Subatomic Physics, Vienna, Austria.C.Adloff68D.BhowmikC.M.KuoW.LinP.K.RoutP.C.Tiwari42S.S.YuNational Central University, Chung-Li, TaiwanNational Central UniversityChung-LiTaiwanNational Central University, Chung-Li, Taiwan68Also at Laboratoire d'Annecy-le-Vieux de Physique des Particules, IN2P3-CNRS, Annecy-le-Vieux, France.L.CeardY.ChaoK.F.ChenP.s.ChenZ.g.ChenW.-S.HouT.h.HsuY.w.KaoR.KhuranaG.KoleY.y.LiR.-S.LuE.PaganisX.f.SuJ.Thomas-WilskerL.s.TsaiH.y.WuE.YazganNational Taiwan University (NTU), Taipei, TaiwanNational Taiwan University (NTU)TaipeiTaiwanNational Taiwan University (NTU), Taipei, TaiwanC.AsawatangtrakuldeeN.SrimanobhasV.WachirapusitanandHigh Energy Physics Research Unit, Department of Physics, Faculty of Science, Chulalongkorn University, Bangkok, ThailandHigh Energy Physics Research UnitDepartment of PhysicsFaculty of ScienceChulalongkorn UniversityBangkokThailandHigh Energy Physics Research Unit, Department of Physics, Faculty of Science, Chulalongkorn University, Bangkok, ThailandD.AgyelF.BoranZ.S.DemirogluF.DolekI.Dumanoglu69E.EskutY.Guler70E.Gurpinar Guler70C.IsikO.KaraA.Kayis TopaksuU.KiminsuG.OnengutK.Ozdemir71A.PolatozB.Tali72U.G.TokS.TurkcaparE.UslanI.S.ZorbakirÇukurova University, Physics Department, Science and Art Faculty, Adana, TurkeyÇukurova UniversityPhysics DepartmentScience and Art FacultyAdanaTurkeyÇukurova University, Physics Department, Science and Art Faculty, Adana, Turkey69Also at Near East University, Research Center of Experimental Health Science, Mersin, Turkey.70Also at Konya Technical University, Konya, Turkey.71Also at Izmir Bakircay University, Izmir, Turkey.72Also at Adiyaman University, Adiyaman, Turkey.M.Yalvac73Middle East Technical University, Physics Department, Ankara, TurkeyMiddle East Technical UniversityPhysics DepartmentAnkaraTurkeyMiddle East Technical University, Physics Department, Ankara, Turkey73Also at Bozok Universitetesi Rektörlügü, Yozgat, Turkey.B.AkgunI.O.AtakisiE.GülmezM.Kaya74O.Kaya75S.Tekten76Bogazici University, Istanbul, TurkeyBogazici UniversityIstanbulTurkeyBogazici University, Istanbul, Turkey74Also at Marmara University, Istanbul, Turkey.75Also at Milli Savunma University, Istanbul, Turkey.76Also at Kafkas University, Kars, Turkey.A.CakirK.Cankocak6977Y.KomurcuS.Sen78Istanbul Technical University, Istanbul, TurkeyIstanbul Technical UniversityIstanbulTurkeyIstanbul Technical University, Istanbul, Turkey77Now at stanbul Okan University, Istanbul, Turkey.78Also at Hacettepe University, Ankara, Turkey.O.AydilekS.Cerci72V.EpshteynB.HacisahinogluI.Hos79B.KaynakS.OzkorucukluO.PotokH.SertC.SimsekD.Sunar Cerci72C.ZorbilmezIstanbul University, Istanbul, TurkeyIstanbul UniversityIstanbulTurkeyIstanbul University, Istanbul, Turkey79Also at Istanbul University - Cerrahpasa, Faculty of Engineering, Istanbul, Turkey.B.Isildak80Yildiz Technical University, Istanbul, TurkeyYildiz Technical UniversityIstanbulTurkeyYildiz Technical University, Istanbul, Turkey80Also at Yildiz Technical University, Istanbul, Turkey.A.BoyaryntsevB.GrynyovInstitute for Scintillation Materials of National Academy of Science of Ukraine, Kharkiv, UkraineInstitute for Scintillation Materials of National Academy of Science of UkraineKharkivUkraineInstitute for Scintillation Materials of National Academy of Science of Ukraine, Kharkiv, UkraineL.LevchukNational Science Centre, Kharkiv Institute of Physics and Technology, Kharkiv, UkraineNational Science CentreKharkiv Institute of Physics and TechnologyKharkivUkraineNational Science Centre, Kharkiv Institute of Physics and Technology, Kharkiv, UkraineD.AnthonyJ.J.BrookeA.BundockF.BuryE.ClementD.CussansH.FlacherM.GlowackiJ.GoldsteinH.F.HeathL.KreczkoS.ParamesvaranS.Seif El Nasr-StoreyV.J.SmithN.Stylianou81K.Walkingshaw PassR.WhiteUniversity of Bristol, Bristol, United KingdomUniversity of BristolBristolUnited KingdomUniversity of Bristol, Bristol, United Kingdom81Also at Vrije Universiteit Brussel, Brussel, Belgium.A.H.BallK.W.BellA.Belyaev82C.BrewR.M.BrownD.J.A.CockerillC.CookeK.V.EllisK.HarderS.HarperM.-L.Holmberg83J.LinacreK.ManolopoulosD.M.NewboldE.OlaiyaD.PetytT.ReisG.SalviT.SchuhC.H.Shepherd-ThemistocleousI.R.TomalinT.WilliamsRutherford Appleton Laboratory, Didcot, United KingdomRutherford Appleton LaboratoryDidcotUnited KingdomRutherford Appleton Laboratory, Didcot, United Kingdom82Also at School of Physics and Astronomy, University of Southampton, Southampton, United Kingdom.83Also at University of Bristol, Bristol, United Kingdom.R.BainbridgeP.BlochC.E.BrownO.BuchmullerV.CacchioC.A.Carrillo MontoyaG.S.Chahal84D.CollingJ.S.DancuI.DasP.DaunceyG.DaviesJ.DaviesM.Della NegraS.FayerG.FediG.HallM.H.HassanshahiA.HowardG.IlesM.KnightJ.LangfordJ.León HolgadoL.LyonsA.-M.MagnanS.MalikA.MartelliM.MieskolainenJ.Nash85M.PesaresiB.C.Radburn-SmithA.RichardsA.RoseC.SeezR.ShuklaA.TapperK.UchidaG.P.UttleyL.H.VageT.Virdee33M.VojinovicN.WardleD.WinterbottomImperial College, London, United KingdomImperial CollegeLondonUnited KingdomImperial College, London, United Kingdom84Also at IPPP Durham University, Durham, United Kingdom.85Also at Monash University, Faculty of Science, Clayton, Australia.K.ColdhamJ.E.ColeA.KhanP.KyberdI.D.ReidBrunel University, Uxbridge, United KingdomBrunel UniversityUxbridgeUnited KingdomBrunel University, Uxbridge, United KingdomS.AbdullinA.BrinkerhoffB.CarawayJ.DittmannK.HatakeyamaJ.HiltbrandB.McMasterM.SaundersS.SawantC.SutantawibulJ.WilsonBaylor University, Waco, TX, USABaylor UniversityWacoTXUSABaylor University, Waco, Texas, USAR.BartekA.DominguezC.Huerta EscamillaA.E.SimsekR.UniyalA.M.Vargas HernandezCatholic University of America, Washington, DC, USACatholic University of AmericaWashingtonDCUSACatholic University of America, Washington, DC, USAB.BamR.ChudasamaS.I.CooperS.V.GleyzerC.U.PerezP.Rumerio86E.UsaiR.YiThe University of Alabama, Tuscaloosa, AL, USAThe University of AlabamaTuscaloosaALUSAThe University of Alabama, Tuscaloosa, Alabama, USA86Also at Università di Torino, Torino, Italy.A.AkpinarA.AlbertD.ArcaroC.CosbyZ.DemiragliC.EriceC.FangmeierC.Fernandez MadrazoE.FontanesiD.GastlerF.GolfS.JeonI.ReedJ.RohlfK.SalyerD.SperkaD.SpitzbartI.SuarezA.TsatsosS.YuanA.G.ZecchinelliBoston University, Boston, MA, USABoston UniversityBostonMAUSABoston University, Boston, Massachusetts, USAG.BenelliX.Coubez28D.CuttsM.HadleyU.HeintzJ.M.Hogan87T.KwonG.LandsbergK.T.LauD.LiJ.LuoS.MondalM.Narain†N.PervanS.Sagir88F.SimpsonM.StamenkovicW.Y.WongX.YanW.ZhangBrown University, Providence, RI, USABrown UniversityProvidenceRIUSABrown University, Providence, Rhode Island, USA87Also at Bethel University, St. Paul, Minnesota, USA.88Also at Karamanoğlu Mehmetbey University, Karaman, Turkey.S.AbbottJ.BonillaC.BrainerdR.BreedonM.Calderon De La Barca SanchezM.ChertokM.CitronJ.ConwayP.T.CoxR.ErbacherF.JensenO.KukralG.MocellinM.MulhearnD.PellettW.WeiY.YaoF.ZhangUniversity of California, Davis, Davis, CA, USAUniversity of California, DavisDavisCAUSAUniversity of California, Davis, Davis, California, USAM.BachtisR.CousinsA.DattaG.Flores AvilaJ.HauserM.IgnatenkoM.A.IqbalT.LamE.MancaA.Nunez Del PradoD.SaltzbergV.ValuevUniversity of California, Los Angeles, CA, USAUniversity of CaliforniaLos AngelesCAUSAUniversity of California, Los Angeles, California, USAR.ClareJ.W.GaryM.GordonG.HansonW.SiS.Wimpenny†University of California, Riverside, Riverside, CA, USAUniversity of California, RiversideRiversideCAUSAUniversity of California, Riverside, Riverside, California, USAJ.G.BransonS.CittolinS.CoopersteinD.DiazJ.DuarteL.GianniniJ.GuiangR.KansalV.KrutelyovR.LeeJ.LettsM.MasciovecchioF.MokhtarS.MukherjeeM.PieriM.QuinnanB.V.Sathia NarayananV.SharmaM.TadelE.VourliotisF.WürthweinY.XiangA.YagilUniversity of California, San Diego, La Jolla, CA, USAUniversity of California, San DiegoLa JollaCAUSAUniversity of California, San Diego, La Jolla, California, USAA.BarzdukasL.BrennanC.CampagnariA.DorsettJ.IncandelaJ.KimA.J.LiP.MastersonH.MeiJ.RichmanU.SaricaR.SchmitzF.SettiJ.SheplockD.StuartT.Á.VámiS.WangUniversity of California, Santa Barbara - Department of Physics, Santa Barbara, CA, USAUniversity of California, Santa BarbaraDepartment of PhysicsSanta BarbaraCAUSAUniversity of California, Santa Barbara - Department of Physics, Santa Barbara, California, USAA.BornheimO.CerriA.LatorreJ.MaoH.B.NewmanM.SpiropuluJ.R.VlimantC.WangS.XieR.Y.ZhuCalifornia Institute of Technology, Pasadena, CA, USACalifornia Institute of TechnologyPasadenaCAUSACalifornia Institute of Technology, Pasadena, California, USAJ.AlisonS.AnM.B.AndrewsP.BryantM.CremonesiV.DuttaT.FergusonA.HarilalC.LiuT.MudholkarS.MurthyM.PauliniA.RobertsA.SanchezW.TerrillCarnegie Mellon University, Pittsburgh, PA, USACarnegie Mellon UniversityPittsburghPAUSACarnegie Mellon University, Pittsburgh, Pennsylvania, USAJ.P.CumalatW.T.FordA.HassaniG.KarathanasisE.MacDonaldN.ManganelliF.MariniA.PerloffC.SavardN.SchonbeckK.StensonK.A.UlmerS.R.WagnerN.ZipperUniversity of Colorado Boulder, Boulder, CO, USAUniversity of Colorado BoulderBoulderCOUSAUniversity of Colorado Boulder, Boulder, Colorado, USAJ.AlexanderS.Bright-ThonneyX.ChenD.J.CranshawJ.FanX.FanD.GadkariS.HoganP.KotamnivesJ.MonroyM.OshiroJ.R.PattersonJ.ReichertM.ReidA.RydJ.ThomP.WittichR.ZouCornell University, Ithaca, NY, USACornell UniversityIthacaNYUSACornell University, Ithaca, New York, USAM.AlbrowM.AlyariO.AmramG.ApollinariA.ApresyanL.A.T.BauerdickD.BerryJ.BerryhillP.C.BhatK.BurkettJ.N.ButlerA.CanepaG.B.CeratiH.W.K.CheungF.ChlebanaG.CummingsJ.DickinsonI.DuttaV.D.ElviraY.FengJ.FreemanA.GandrakotaZ.GecseL.GrayD.GreenA.GrummerS.GrünendahlD.GuerreroO.GutscheR.M.HarrisR.HellerT.C.HerwigJ.HirschauerL.HorynB.JayatilakaS.JindarianiM.JohnsonU.JoshiT.KlijnsmaB.KlimaK.H.M.KwokS.LammelD.LincolnR.LiptonT.LiuC.MadridK.MaeshimaC.MantillaD.MasonP.McBrideP.MerkelS.MrennaS.NahnJ.NgadiubaD.NoonanV.PapadimitriouN.PastikaK.PedroC.Pena89F.RaveraA.Reinsvold Hall90L.RistoriE.Sexton-KennedyN.SmithA.SohaL.SpiegelS.StoynevJ.StraitL.TaylorS.TkaczykN.V.TranL.UpleggerE.W.VaanderingI.ZoiFermi National Accelerator Laboratory, Batavia, IL, USAFermi National Accelerator LaboratoryBataviaILUSAFermi National Accelerator Laboratory, Batavia, Illinois, USA89Also at California Institute of Technology, Pasadena, California, USA.90Also at United States Naval Academy, Annapolis, Maryland, USA.C.ArutaP.AveryD.BourilkovL.CadamuroP.ChangV.CherepanovR.D.FieldE.KoenigM.KolosovaJ.KonigsbergA.KorytovK.H.LoK.MatchevN.MenendezG.MitselmakherK.MohrmanA.Muthirakalayil MadhuN.RawalD.RosenzweigS.RosenzweigK.ShiJ.WangUniversity of Florida, Gainesville, FL, USAUniversity of FloridaGainesvilleFLUSAUniversity of Florida, Gainesville, Florida, USAT.AdamsA.Al KadhimA.AskewN.BowerR.HabibullahV.HagopianR.HashmiR.S.KimS.KimT.KolbergG.MartinezH.ProsperP.R.ProvaO.ViazloM.WulansatitiR.YohayJ.ZhangFlorida State University, Tallahassee, FL, USAFlorida State UniversityTallahasseeFLUSAFlorida State University, Tallahassee, Florida, USAB.AlsufyaniM.M.BaarmandS.ButallaT.Elkafrawy56M.HohlmannR.Kumar VermaM.RahmaniE.YanesFlorida Institute of Technology, Melbourne, FL, USAFlorida Institute of TechnologyMelbourneFLUSAFlorida Institute of Technology, Melbourne, Florida, USAM.R.AdamsA.BatyC.BennettR.CavanaughS.DittmerR.Escobar FrancoO.EvdokimovC.E.GerberD.J.HofmanJ.h.LeeD.S.LemosA.H.MerritC.MillsS.NandaG.OhB.OzekD.PilipovicR.PradhanT.RoyS.RudrabhatlaM.B.TonjesN.VarelasX.WangZ.YeJ.YooUniversity of Illinois Chicago, Chicago, USAUniversity of Illinois ChicagoChicagoUSAUniversity of Illinois Chicago, Chicago, USA, Chicago, USAM.AlhusseiniD.BlendK.Dilsiz91L.EmediatoG.KaramanO.K.KöseyanJ.-P.MerloA.Mestvirishvili92J.NachtmanO.NeogiH.Ogul93Y.OnelA.PenzoC.SnyderE.Tiras94The University of Iowa, Iowa City, IA, USAThe University of IowaIowa CityIAUSAThe University of Iowa, Iowa City, Iowa, USA91Also at Bingol University, Bingol, Turkey.92Also at Georgian Technical University, Tbilisi, Georgia.93Also at Sinop University, Sinop, Turkey.94Also at Erciyes University, Kayseri, Turkey.B.BlumenfeldL.CorcodilosJ.DavisA.V.GritsanL.KangS.KyriacouP.MaksimovicM.RoguljicJ.RoskesS.SekharM.SwartzJohns Hopkins University, Baltimore, MD, USAJohns Hopkins UniversityBaltimoreMDUSAJohns Hopkins University, Baltimore, Maryland, USAA.AbreuL.F.Alcerro AlcerroJ.AnguianoP.BaringerA.BeanZ.FlowersD.GroveJ.KingG.KrintirasM.LazarovitsC.Le MahieuC.LindseyJ.MarquezN.MinafraM.MurrayM.NickelM.PittS.Popescu95C.RoganC.RoyonR.SalvaticoS.SandersC.SmithQ.WangG.WilsonThe University of Kansas, Lawrence, KS, USAThe University of KansasLawrenceKSUSAThe University of Kansas, Lawrence, Kansas, USA95Also at Horia Hulubei National Institute of Physics and Nuclear Engineering (IFIN-HH), Bucharest, Romania.B.AllmondA.IvanovK.KaadzeA.KalogeropoulosD.KimY.MaravinK.NamJ.NatoliD.RoyG.SorrentinoKansas State University, Manhattan, KS, USAKansas State UniversityManhattanKSUSAKansas State University, Manhattan, Kansas, USAF.RebassooD.WrightLawrence Livermore National Laboratory, Livermore, CA, USALawrence Livermore National LaboratoryLivermoreCAUSALawrence Livermore National Laboratory, Livermore, California, USAA.BadenA.BelloniA.BethaniY.M.ChenS.C.EnoN.J.HadleyS.JabeenR.G.KelloggT.KoethY.LaiS.LascioA.C.MignereyS.NabiliC.PalmerC.PapageorgakisM.M.ParanjpeL.WangUniversity of Maryland, College Park, MD, USAUniversity of MarylandCollege ParkMDUSAUniversity of Maryland, College Park, Maryland, USAJ.BendavidW.BuszaI.A.CaliY.ChenM.D'AlfonsoJ.EysermansC.FreerG.Gomez-CeballosM.GoncharovG.GrossoP.HarrisD.HoangD.KovalskyiJ.KrupaL.LavezzoY.-J.LeeK.LongC.MironovC.PausD.RankinC.RolandG.RolandS.RothmanZ.ShiG.S.F.StephansZ.WangB.WyslouchT.J.YangMassachusetts Institute of Technology, Cambridge, MA, USAMassachusetts Institute of TechnologyCambridgeMAUSAMassachusetts Institute of Technology, Cambridge, Massachusetts, USAB.CrossmanB.M.JoshiC.KapsiakM.KrohnD.MahonJ.MansB.MarzocchiS.PandeyM.ReveringR.RusackR.SaradhyN.SchroederN.StrobbeM.A.WadudUniversity of Minnesota, Minneapolis, MN, USAUniversity of MinnesotaMinneapolisMNUSAUniversity of Minnesota, Minneapolis, Minnesota, USAL.M.CremaldiUniversity of Mississippi, Oxford, MS, USAUniversity of MississippiOxfordMSUSAUniversity of Mississippi, Oxford, Mississippi, USAK.BloomM.BrysonD.R.ClaesG.HazaJ.HossainC.JooI.KravchenkoJ.E.SiadoW.TabbA.VagneriniA.WightmanF.YanD.YuUniversity of Nebraska-Lincoln, Lincoln, NE, USAUniversity of Nebraska-LincolnLincolnNEUSAUniversity of Nebraska-Lincoln, Lincoln, Nebraska, USAH.BandyopadhyayL.HayI.IashviliA.KharchilavaM.MorrisD.NguyenS.RappoccioH.Rejeb SfarA.WilliamsState University of New York at Buffalo, Buffalo, NY, USAState University of New York at BuffaloBuffaloNYUSAState University of New York at Buffalo, Buffalo, New York, USAG.AlversonE.BarberisJ.DervanY.HaddadY.HanA.KrishnaJ.LiM.Lu96G.MadiganR.MccarthyD.M.MorseV.NguyenT.OrimotoA.ParkerL.SkinnariA.Tishelman-CharnyB.WangD.WoodNortheastern University, Boston, MA, USANortheastern UniversityBostonMAUSANortheastern University, Boston, Massachusetts, USA96Also at Sun Yat-Sen University, Guangzhou, China.S.BhattacharyaJ.BueghlyZ.ChenK.A.HahnY.LiuY.MiaoD.G.MonkM.H.SchmittA.TaliercioM.VelascoNorthwestern University, Evanston, IL, USANorthwestern UniversityEvanstonILUSANorthwestern University, Evanston, Illinois, USAG.AgarwalR.BandR.BucciS.CastellsA.DasR.GoldouzianM.HildrethK.W.HoK.Hurtado AnampaT.IvanovC.JessopK.LannonJ.LawrenceN.LoukasL.LuttonJ.MarianoN.MarinelliI.McalisterT.McCauleyC.McgradyC.MooreY.Musienko17H.NelsonM.OshersonA.PiccinelliR.RuchtiA.TownsendY.WanM.WayneH.YockeyM.ZaruckiL.ZygalaUniversity of Notre Dame, Notre Dame, IN, USAUniversity of Notre DameNotre DameINUSAUniversity of Notre Dame, Notre Dame, Indiana, USAA.BasnetB.BylsmaM.CarriganL.S.DurkinC.HillM.JoyceM.Nunez OrnelasK.WeiB.L.WinerB.R.YatesThe Ohio State University, Columbus, OH, USAThe Ohio State UniversityColumbusOHUSAThe Ohio State University, Columbus, Ohio, USAF.M.AddesaH.BouchamaouiP.DasG.DezoortP.ElmerA.FrankenthalB.GreenbergN.HaubrichG.KoppS.KwanD.LangeA.LoeligerD.MarlowI.OjalvoJ.OlsenA.ShevelevD.SticklandC.TullyPrinceton University, Princeton, NJ, USAPrinceton UniversityPrincetonNJUSAPrinceton University, Princeton, New Jersey, USAS.MalikUniversity of Puerto Rico, Mayaguez, PR, USAUniversity of Puerto RicoMayaguezPRUSAUniversity of Puerto Rico, Mayaguez, Puerto Rico, USAA.S.BakshiV.E.BarnesS.ChandraR.ChawlaS.DasA.GuL.GutayM.JonesA.W.JungD.KondratyevA.M.KoshyM.LiuG.NegroN.NeumeisterG.PaspalakiS.PiperovV.ScheurerJ.F.SchulteM.StojanovicJ.ThiemanA.K.VirdiF.WangW.XiePurdue University, West Lafayette, IN, USAPurdue UniversityWest LafayetteINUSAPurdue University, West Lafayette, Indiana, USAJ.DolenN.ParasharA.PathakPurdue University Northwest, Hammond, IN, USAPurdue University NorthwestHammondINUSAPurdue University Northwest, Hammond, Indiana, USAD.AcostaT.CarnahanK.M.EcklundP.J.Fernández MantecaS.FreedP.GardnerF.J.M.GeurtsW.LiO.Miguel ColinB.P.PadleyR.RedjimiJ.RotterE.YigitbasiY.ZhangRice University, Houston, TX, USARice UniversityHoustonTXUSARice University, Houston, Texas, USAA.BodekP.de BarbaroR.DeminaJ.L.DulembaC.FallonA.Garcia-BellidoO.HindrichsA.KhukhunaishviliN.ParmarP.Parygin34E.Popova34R.TausG.P.Van OnsemUniversity of Rochester, Rochester, NY, USAUniversity of RochesterRochesterNYUSAUniversity of Rochester, Rochester, New York, USAK.GoulianosThe Rockefeller University, New York, NY, USAThe Rockefeller UniversityNew YorkNYUSAThe Rockefeller University, New York, New York, USAB.ChiaritoJ.P.ChouY.GershteinE.HalkiadakisA.HartM.HeindlD.JaroslawskiO.Karacheban31I.LaflotteA.LathR.MontalvoK.NashH.RoutrayS.SalurS.SchnetzerS.SomalwarR.StoneS.A.ThayilS.ThomasJ.VoraH.WangRutgers, The State University of New Jersey, Piscataway, NJ, USARutgers, The State University of New JerseyPiscatawayNJUSARutgers, The State University of New Jersey, Piscataway, New Jersey, USAH.AcharyaD.AllyA.G.DelannoyS.FiorendiS.HigginbothamT.HolmesA.R.KanugantiN.KarunarathnaL.LeeE.NibigiraS.SpanierUniversity of Tennessee, Knoxville, TN, USAUniversity of TennesseeKnoxvilleTNUSAUniversity of Tennessee, Knoxville, Tennessee, USAD.AebiM.AhmadO.Bouhali97M.DalchenkoR.EusebiJ.GilmoreT.HuangT.Kamon98H.KimS.LuoS.MalhotraR.MuellerD.OvertonD.RathjensA.SafonovTexas A&M University, College Station, TX, USATexas A&M UniversityCollege StationTXUSATexas A&M University, College Station, Texas, USA97Also at Texas A&M University at Qatar, Doha, Qatar.98Also at Kyungpook National University, Daegu, Korea.N.AkchurinJ.DamgovV.HegdeA.HussainY.KazhykarimK.LamichhaneS.W.LeeA.MankelT.PeltolaI.VolobouevA.WhitbeckTexas Tech University, Lubbock, TX, USATexas Tech UniversityLubbockTXUSATexas Tech University, Lubbock, Texas, USAE.AppeltS.GreeneA.GurrolaW.JohnsR.Kunnawalkam ElayavalliA.MeloF.RomeoP.SheldonS.TuoJ.VelkovskaJ.ViinikainenVanderbilt University, Nashville, TN, USAVanderbilt UniversityNashvilleTNUSAVanderbilt University, Nashville, Tennessee, USAB.CardwellB.CoxJ.HakalaR.HiroskyA.LedovskoyC.NeuC.E.Perez LaraUniversity of Virginia, Charlottesville, VA, USAUniversity of VirginiaCharlottesvilleVAUSAUniversity of Virginia, Charlottesville, Virginia, USAP.E.KarchinWayne State University, Detroit, MI, USAWayne State UniversityDetroitMIUSAWayne State University, Detroit, Michigan, USAA.AravindS.BanerjeeK.BlackT.BoseS.DasuI.De BruynP.EveraertsC.GalloniH.HeM.HerndonA.HerveC.K.KorakaA.LanaroR.LovelessJ.Madhusudanan SreekalaA.MallampalliA.MohammadiS.MondalG.ParidaD.PinnaA.SavinV.ShangV.SharmaW.H.SmithD.TeagueH.F.TsoiW.VetensA.WardenUniversity of Wisconsin - Madison, Madison, WI, USAUniversity of Wisconsin - MadisonMadisonWIUSAUniversity of Wisconsin - Madison, Madison, Wisconsin, USAS.AfanasievV.AndreevYu.AndreevT.AushevM.AzarkinA.BabaevA.BelyaevV.Blinov99E.BoosV.BorshchD.BudkouskiV.BunichevV.ChekhovskyR.Chistov99M.Danilov99A.DermenevT.Dimova99D.Druzhkin100M.Dubinin89L.DudkoA.ErshovG.GavrilovV.GavrilovS.GninenkoV.GolovtcovN.GolubevI.GolutvinI.GorbunovA.GribushinY.IvanovV.KachanovV.KarjavineA.KarneyeuV.Kim99M.KirakosyanD.KirpichnikovM.KirsanovV.KlyukhinV.KorenkovA.Kozyrev99N.KrasnikovA.LanevP.Levchenko101N.LychkovskayaV.MakarenkoA.MalakhovV.Matveev99V.MurzinA.Nikitenko102103S.ObraztsovV.OreshkinV.PalichikV.PerelyginM.PerfilovS.Polikarpov99V.PopovO.Radchenko99M.SavinaV.SavrinV.ShalaevS.ShmatovS.ShulhaY.Skovpen99S.SlabospitskiiV.SmirnovD.SosnovV.SulimovE.TcherniaevA.TerkulovO.TeryaevI.TlisovaA.ToropinL.UvarovA.UzunianP.VolkovA.Vorobyev†G.VorotnikovN.VoytishinB.S.Yuldashev104A.ZarubinI.ZhizhinA.ZhokinAuthors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERNAuthors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERNAuthors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN99Also at another institute or international laboratory covered by a cooperation agreement with CERN.100Also at Universiteit Antwerpen, Antwerpen, Belgium.101Also at Northeastern University, Boston, Massachusetts, USA.102Also at Imperial College, London, United Kingdom.103Now at Yerevan Physics Institute, Yerevan, Armenia.104Also at Institute of Nuclear Physics of the Uzbekistan Academy of Sciences, Tashkent, Uzbekistan.CERN, Geneva, SwitzerlandCERNGenevaSwitzerlandCERN, Geneva, Switzerland⋆E-mail address:cms-publication-committee-chair@cern.ch.Editor: M. DoserAbstractA search is presented for new Higgs bosons in proton-proton (pp) collision events in which a same-sign top quark pair is produced in association with a jet, via the pp→tH/A→ttc‾ and pp→tH/A→ttu‾ processes. Here, H and A represent the extra scalar and pseudoscalar boson, respectively, of the second Higgs doublet in the generalized two-Higgs-doublet model (g2HDM). The search is based on pp collision data collected at a center-of-mass energy of 13 TeV with the CMS detector at the LHC, corresponding to an integrated luminosity of 138fb−1. Final states with a same-sign lepton pair in association with jets and missing transverse momentum are considered. New Higgs bosons in the 200–1000 GeV mass range and new Yukawa couplings between 0.1 and 1.0 are targeted in the search, for scenarios in which either H or A appear alone, or in which they coexist and interfere. No significant excess above the standard model prediction is observed. Exclusion limits are derived in the context of the g2HDM.KeywordsCMSTop quarksExtra Higgs bosonYukawa couplingsData availabilityRelease and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS policy as stated in “CMS data preservation, re-use and open access policy”.1IntroductionUsing proton-proton (pp) collision data recorded during the CERN LHC Run 1 (2011–2012) data-taking period, the ATLAS and CMS experiments discovered a scalar boson, h125, with a mass of 125 GeV, the properties of which are so far consistent with those of the Higgs boson of the standard model (SM) [1–3]. The analysis of the additional Run 2 (2015–2018) data enabled more precise measurements of the Higgs boson properties and further constrained the possible contributions from new physics beyond the SM [4,5]. The ATLAS and CMS experiments have measured the Yukawa couplings of the h125 boson to the t and b quarks, and the τ and μ leptons [6,7]. In all cases, the couplings are found to be consistent with the SM expectations within uncertainties.Having established the existence of one scalar SU(2) doublet, natural questions emerge about the possibility of additional doublets. A second doublet is predicted in two-Higgs-doublet models (2HDM), resulting in five physical scalar bosons: CP-even neutral scalar bosons h and H with mH>mh, a CP-odd pseudoscalar boson A, and two charged Higgs bosons H±[8]. These additional Higgs bosons at mass scales ≲1TeV may still exist within the reach of the LHC [9], but their signatures may be suppressed by fermion mass-mixing hierarchy [10] or alignment mechanisms, where the mixing angle γ between the two CP-even scalar bosons h and H has a value for which cos⁡γ≈0[11]. In the alignment limit [12–14], the lightest scalar boson h becomes the SM h125 boson, and the extra spin-0 bosons do not interact with vector boson pairs (i.e., HVV and AVV interactions do not occur, where V is a W or Z boson). Alignment suppresses flavor changing neutral current interactions of the h boson but allows them for the H and A bosons. Therefore, the lack of a hint of the processes such as t→ch125/uh125 or h125→μτ/eτ at the LHC may be because their amplitudes are suppressed by alignment. As shown in Ref. [11], the alignment scenario may occur if all extra Higgs quartic couplings are O(1) and no Z2 symmetry requirement is imposed, allowing flavor changing neutral Higgs couplings involving H and A bosons. This scenario without Z2 symmetry can be studied in the framework of the generalized 2HDM (g2HDM) [8,10,15], with new Yukawa couplings such as ρτμ, ρtu, ρtc, and ρtt that may assume significantly large values [8,10,15]. These new Yukawa couplings combined with Higgs quartic couplings of ≈1 may also explain the electroweak baryogenesis [16,17] and therefore the disappearance of antimatter soon after the Big Bang. The new top Yukawa coupling ρtc with a similar strength to ρτμ may be compatible with the observed data depending on the H± mass, which may also explain a possible muon g−2 anomaly [18]. These arguments strongly motivate to verify with direct experimental searches whether new Yukawa couplings exist. The processes discussed above have been recently explored by the ATLAS experiment [19].In this Letter, we present a search for the existence of the real part of these couplings, ρtu and ρtc, through the pp→tH/A→ttq‾(q=u,c) and the charge conjugate processes, considering one coupling at a time and keeping the other at zero using the Run 2 data set recorded by the CMS experiment. A representative Feynman diagram for the ttq‾ process is displayed in Fig. 1. The final-state signature for ttq‾ explored in this Letter consists of two same-sign (SS) leptons with at least three jets, two of which are identified as b jets and one compatible with originating from a u or c quark, and missing transverse momentum. The main background consists of events with nonprompt leptons originating from leptonic decays of heavy quarks, hadrons misidentified as leptons, electrons from photon conversions, or jets misidentified as leptons.The analysis is performed using pp collision data at a center-of-mass energy of 13 TeV. The data were collected with the CMS detector at the LHC between 2016 and 2018, and correspond to an integrated luminosity of 138fb−1. Tabulated results are accessible from the HEPData record for this analysis [20].The Letter is organized as follows: Section 2 describes the CMS detector, along with object reconstruction. In Section 3, a description of the simulation samples used in the analysis is given. The event selection and reconstruction procedure of the physics objects are given in Section 4. Following, in Section 5, the signal extraction procedure is explained. Section 6 discusses the sources of systematic uncertainties. The results of the analysis are presented in Section 7. Finally, a summary of the analysis is given in Section 8.2The CMS detector and object reconstructionThe CMS apparatus [21] is a multipurpose, nearly hermetic detector, designed to trigger on [22,23] and identify electrons, muons, photons, and (charged and neutral) hadrons [24–26]. A global “particle-flow” (PF) algorithm [27] aims to reconstruct all individual particles in an event, combining information provided by the all-silicon inner tracker and by the crystal electromagnetic (ECAL) and brass-scintillator hadron calorimeters (HCAL), operating inside a 3.8 T superconducting solenoid, with data from the gas-ionization muon detectors embedded in the flux-return yoke outside the solenoid.The primary vertex is taken to be the vertex corresponding to the hardest scattering in the event, evaluated using tracking information alone, as described in Section 9.4.1 of Ref. [28]. The energy of photons is obtained from the ECAL measurement. The energy of electrons is determined from a combination of the electron momentum at the primary interaction vertex as determined by the tracker, the energy of the corresponding ECAL cluster, and the energy sum of all bremsstrahlung photons spatially compatible with originating from the electron track. The energy of muons is obtained from the curvature of the corresponding track. The energy of charged hadrons is determined from a combination of their momentum measured in the tracker and the matching ECAL and HCAL energy deposits, corrected for the response function of the calorimeters to hadronic showers. Finally, the energy of neutral hadrons is obtained from the corresponding corrected ECAL and HCAL energies.Jets are built from PF particles using the anti-kT algorithm [29,30] with a distance parameter of 0.4. Jet momentum is determined as the vectorial sum of all particle momenta in the jet, and is found from simulation to be, on average, within 5 to 10% of the true momentum over the whole pT spectrum and detector acceptance. Additional pp interactions within the same or nearby bunch crossings can contribute additional tracks and calorimetric energy depositions, increasing the apparent jet momentum. To mitigate this effect, tracks identified to be originating from the multiple pp interactions occurring in the same or nearby bunch crossings (pileup) are discarded and an offset correction is applied to correct for remaining contributions [31]. Jet energy corrections are derived from simulation studies so that the average measured energy of jets becomes identical to that of particle level jets. In situ measurements of the momentum balance in dijet, photon+jet, Z+jets, and multijet events are used to determine any residual differences between the jet energy scale in data and in simulation, and appropriate corrections are made [32]. Additional selection criteria are applied to each jet to remove jets potentially dominated by instrumental effects or reconstruction failures [31]. The missing transverse momentum vector p→Tmiss is computed as the negative vector sum of the transverse momenta of all the PF candidates in an event, and its magnitude is denoted as pTmiss[33]. The p→Tmiss is modified to account for corrections to the energy scale of the reconstructed jets in the event.Events of interest are selected using a two-tiered trigger system. The first level (L1), composed of custom hardware processors, uses information from the calorimeters and muon detectors to select events at a rate of around 100 kHz within a fixed latency of about 4μs[22]. The second level, known as the high-level trigger, consists of a farm of processors running a version of the full event reconstruction software optimized for fast processing, and reduces the event rate to around 1 kHz before data storage [23].3Simulated event samplesThe signal and background processes are simulated using several Monte Carlo (MC) programs. The ttq‾ signal samples are simulated at leading order (LO) in perturbative quantum chromodynamics (QCD) with up to two additional noncollinear high-pT partons using MadGraph5_amc@nlo 2.6.5 [34], and the hard-process simulation is interfaced with parton shower jets using the MLM [35] matching prescription. Different signal samples are simulated for the case where a mass between 200 and 1000 GeV is assumed for A (H), and a mass too high to be of reach for our search is assumed for H (A). For these signal samples, there is no interference between A and H. Signal samples are also generated for the case where both A and H coexist and interfere assuming a mass difference mA−mH=50GeV, following Ref. [36]. The amplitudes for the processes qg→tA→ttq‾ and qg→tH→ttq‾ cancel when A and H are mass degenerate. The signal cross section is not significantly modified with respect to the noninterference case when the mass differences are larger than ≈100GeV. Therefore, the investigated mass difference is chosen to retain some interference effects along with reasonably high cross sections. Depending on the coupling value and the interference assumption we consider in this Letter, the cross sections for the ttu‾ process range from ≈1×10−4 to ≈7×10−1pb and for ttc‾ range from ≈5×10−6 to ≈7×10−2pb, as calculated with MadGraph5_amc@nlo at LO precision in QCD. The inclusive cross section for the ttq‾ process does not change, within uncertainties, when the intermediary particle is H or A, when there is no A-H interference.Background events generated by the MadGraph5_amc@nlo generator are tt‾V, V+jets, tt‾VV, tt‾VH, tZ, tt‾tj, tt‾tW, tt‾tt‾, WZ, vector boson scattering (VBS, i.e., Wℓℓqq or V±V±JJ), VVV, and single top quark s-channel production. Among these processes, FxFx matching [37] is used for tt‾W, Z+jets, and the QCD part of WZ production, while MLM matching [35] is used for W+jets. The powheg 2.0 generator [38–40] is used to simulate events at next-to-LO in perturbative QCD for tt‾[41], ZZ and W±W∓[42], single top quark tW [43] and t-channel [44], and tt‾H production [45].Both the signal and background samples are interfaced with pythia v8.240 [46] for parton showering, fragmentation, and hadronization. The underlying event is also modeled with pythia, using the CP5 tune [47]. The parton distribution functions (PDFs) are taken from the NNPDF3.1 next-to-next-to-LO set [48]. Finally, for both signal and background MC event samples, the detector response is modeled with the Geant4 package [49]. The simulated events are weighted to match the observables sensitive to pileup to those observed in the data [31].The simulated events are corrected for the differences between data and simulation of the trigger efficiencies, lepton identification, and lepton isolation. The corrections are determined using the “tag-and-probe” method applied on Z boson candidate events [50] and are parametrized as functions of the lepton pT and pseudorapidity (η).4Event reconstruction and selectionData are selected online with a combination of double lepton triggers and single lepton triggers to enhance signal efficiency. Charged leptons (electrons or muons) are required to originate from the primary vertex to reject contributions from pileup. Identification of electrons makes use of a multivariate discriminant [51,52] combining observables sensitive to the matching of charged-particle tracks in the tracker to the energy deposits in the ECAL and the amount of bremsstrahlung photons emitted along their trajectory [24]. The number of electrons originating from asymmetric photon conversions is reduced by requiring that their associated track has no missing hits in the innermost layers of the silicon tracker. To ensure the correct assignment of the electric charge of the electrons, further selection criteria were applied [53]. The separation of prompt leptons from nonprompt leptons reconstructed within jets is achieved by using an isolation variable, relative to the lepton pT. The isolation variable is constructed from the scalar pT sum of charged hadrons, neutral hadrons, and photons reconstructed within a cone of variable size that depends on the lepton pT[54]. “Loose” leptons are those that pass the kinematic selection criteria of pT>10GeV and |η|<2.5(2.4) for electrons (muons). Electrons that fall in the region between the ECAL barrel and endcaps (1.442<|η|<1.556) are vetoed. “Tight” leptons are in addition required to have pT>20GeV. A multivariate discriminant is furthermore used to separate prompt leptons and nonprompt leptons originating from the decays of hadrons inside jets, hadrons misidentified as leptons, and electrons from photon conversions. The jets must have pT>30GeV and |η|<2.4 to be considered. In addition, they are required to be separated from identified leptons by ΔR=(Δη)2+(Δϕ)2>0.4, where ϕ is the azimuthal angle measured in radians. At least three jets, and pTmiss>30GeV are required in each event. Jets from the hadronization of b quarks (b jets), c quarks (c jets), and light (i.e., light-quark or gluon) jets are distinguished through the ratios of the corresponding jet flavor probabilities, defined as CvsL (c vs light quark) and CvsB (c vs b quark) [55,56], respectively. These probabilities are obtained from the DeepJet[57,58] algorithm: a neural network utilizing global variables, charged, neutral particle and secondary vertex features in a jet to perform flavor tagging. The differences of the shapes of the CvsL and CvsB discriminant distributions between data and simulation are corrected by flavor-dependent scale factors.The search is performed in three SS dilepton categories: e±e±, μ±μ±, and e±μ±. The event selection ensures complete orthogonality of these three categories to avoid any possible double counting of events selected in the analysis. Events are required to have two tight leptons with the same electric charge for which the leading lepton has pT>30GeV and subleading lepton pT>20GeV. Events containing a third lepton are vetoed if the additional lepton passes the loose selection. The two leptons are required to be separated by ΔR(ℓ1,ℓ2)>0.3 and required to have an invariant mass m(ℓ1,ℓ2)>20GeV. Events with 60<m(ℓ1,ℓ2)<120GeV in the e±e± channel are vetoed to suppress the Drell-Yan (DY) background contribution, the main source of charge misidentified leptons. This veto reduces the selected number of DY events in simulation by about 94% after the aforementioned requirements. This veto is not applied to the e±μ± and μ±μ± channels, as the charge misidentification rate for muons is negligible. The CvsL and CvsB distributions for the leading jet obtained from simulated events and data are displayed in Fig. 2.The nonprompt-lepton background is estimated from control regions in the data using the fake-factor method [59]. A dijet enriched sample is selected from data, from which the probability fp for a loose nonprompt lepton (originating from a jet) to also pass the tight lepton selection criteria is estimated in bins of pT and |η|. The nonprompt-lepton background contribution is then estimated by applying fp to events in a data control sample in which at least one lepton fails the tight lepton selection criteria. A data-driven approach is followed to evaluate the lepton charge misidentification rate in the e±e± channel using DY events with same- and opposite-sign electric charges. It is estimated in bins of lepton pT and η, and is used to calibrate simulated events. The rate, which increases with pT and η, varies from ≈10−5 to ≈10−2.5Signal extractionA boosted decision tree (BDT) discriminant [60] is used to separate signal and background events. We train the BDT model in the signal region, where process yields of both backgrounds and signal are small. For the training, we combine the inputs from different channels. By comparing the BDT output distributions for the training and test samples, we found no evidence of overtraining. We use an optimized set of input observables, listed in Table 1, for our signal topology. Flavor tagging variables are used to differentiate b quarks originating from the top quark decay, and to differentiate c quark and light-quark jets. Pairwise kinematic variables related to jets are incorporated that are sensitive to the resonance structures, specifically to top quarks and A/H. Other kinematic features, such as HT and pTmiss, are also sensitive to our signal and are included. To mitigate the impact of resonances such as the DY process, the dilepton (+jets) invariant mass is also used as an input to the BDT.We use half of the available simulated events for the BDT training. The main backgrounds in the signal region are tt‾ (fully leptonic decay of the top quark-antiquark pair where one lepton has a misidentified charge), nonprompt leptons (dominated by semileptonic tt‾ decay), tt‾W, and tt‾H. In the signal extraction, we use events from data to estimate the nonprompt-lepton background contribution, but we do not use these events for training. Instead, we use simulated samples of semileptonically decaying tt‾ events for the BDT training, to mimic the misidentified lepton in the nonprompt-lepton background. We do not include events from W+jets or single top quark simulation, due to a limited number of simulated events. The various backgrounds are added corresponding to their cross sections. The MC event samples used for the BDT training are ttc‾ or ttu‾ signal, semileptonic tt‾, dileptonic tt‾ (tt‾), tt‾V, VV, VVV, tt‾H, tt‾VH, tt‾VV, tt‾tj, tt‾tW, tt‾tt‾, and VBS. Three values for the couplings ρtu and ρtc, namely, 0.1, 0.4, and 1.0 are considered. For each coupling, ten mA points are considered: 200, 300, 350, 400, 500, 600, 700, 800, 900, and 1000 GeV. Using the same coupling assumptions, we also consider the more realistic case with the A-H interference assuming a fixed mass difference mA−mH=50GeV, with the following nine mA-mH combinations; 250-200, 300-250, 350-300, 400-350, 550-500, 700-650, 800-750, 900-850, and 1000-950 GeV. The signal extraction is performed using the shape of the BDT discriminant distributions. Because of the kinematic differences and different background compositions, the BDTs are trained independently for four data-taking periods, two in 2016, and one for each of the years 2017 and 2018; for each mass assumption, namely for each mA either with no H present or with A-H interference; and for ρtu=0.4 and ρtc=0.4. Therefore, a total of 152 BDTs are trained. The values of the BDT hyperparameters, as defined in the TMVA package [61], are chosen after scanning a range of values, avoiding overtraining, and requiring a high background rejection rate while maintaining a high signal efficiency. We use these same model parameters for all three years of data taking. The BDTs offer high background rejection, while simultaneously maintaining a high signal efficiency. For instance, when considering ρtc=0.4, and a signal efficiency of 96%, the background rejection rates for mA=200GeV and 1000GeV are 50% and 76%, respectively.The signal strength parameter, μ, is obtained using a simultaneous maximum likelihood fit [62], in analyses performed for three decay modes and for four different eras (i.e. 12 categories) for each signal mass-coupling assumption independently. It is defined as μ=σ/σtheory, where σtheory is the predicted ttq‾ production cross section in g2HDM calculated with MadGraph5_amc@nlo +pythia, and σ is the upper limit on the observed cross section. To ensure numerical stability, the bin width is chosen to have a high enough yield in each bin of the BDT distributions. The BDT distribution ranges from −1 to 1, but to reduce the impact on the fit of background-dominated regions, events are selected with a BDT score >−0.6. This requirement on the BDT score also helps to improve the stability of the fit and the corresponding fit uncertainties. Except for the dominant nonprompt-lepton background, the predicted yields and the shapes of the BDT distributions are taken directly from the simulation. When performing the maximum likelihood fit, individual templates are used for the VBS, VV, tt‾ (fully leptonic decays), tt‾H, tt‾W, and nonprompt-lepton background processes, while a combined template labeled others uses a combination of background processes, namely: DY, tt‾VV, tt‾VH, tt‾Z, tt‾tj, tt‾tW, tt‾tt‾, VVV, tZq, tW, and t‾W.6Systematic uncertaintiesSystematic uncertainties, arising from various sources, such as detector effects, theoretical uncertainties, and mismodeling, are evaluated and categorized in two main groups: experimental uncertainties and modeling uncertainties. Several effects modify the event yields or shapes of the measured distributions. The systematic uncertainties are modeled as nuisance parameters in the maximum likelihood estimation procedure used for determining the best fit signal strength μˆ. The nuisance parameters are allowed to modify the shape and normalization of the backgrounds and signal in the fit using the method in Ref. [62]. The chosen probability density function (pdf) used for the interpolation between nominal and systematic templates is dependent on whether the associated nuisance parameter can also affect the shape of the nominal template or not. Log-normal pdfs are used for nuisance parameters that only affect the distributions normalization, whereas Gaussian distributions are used for those that can affect the shape as well. Experimental uncertainties, where appropriate, and all modeling uncertainties are taken as correlated across years and channels. The effect of the limited number of simulated events is estimated using the Barlow–Beeston-lite method [63].The experimental uncertainties are those related to the integrated luminosity [64–66], pileup, L1 trigger inefficiency, nonprompt-lepton background estimation, jet energy scale and resolution, unclustered energy scale, lepton identification and trigger efficiencies, charge misidentification, muon momentum scale, and heavy-quark, light-quark and gluon jet identification. The dominant experimental uncertainty sources are related to the flavor tagger discriminant shape calibration, and nonprompt-lepton background estimation. The modeling uncertainty sources are matrix-element renormalization and factorization scales, parton shower scales that control the initial- and final-state radiation, and PDFs. For the signal, these are included as separate nuisance parameters that affect the shape. For the backgrounds estimated using MC event samples, nuisance parameters are assumed to only affect the yields, and the corresponding uncertainties in the theoretical cross section calculations are used. The most significant modeling uncertainty in the analysis is attributed to the normalization of the tt‾W background, regardless of the A-H interference. The contributions of all uncertainty sources on the pre-fit expected event yields are displayed in Table 2, for ρtc=0.4 and mA=350GeV with A-H interference assuming mA−mH=50GeV. The uncertainties in other scenarios are similar.7ResultsFig. 3 displays the post-fit BDT discriminant distributions used for the signal extraction combining the categories e±e±, μ±μ±, and e±μ±, and for ρtu=1.0 and ρtc=1.0 with A-H interference, assuming mA=350GeV.No significant excess over the expected SM background is observed. The results of the search are interpreted in terms of the upper limits on the signal strength parameter μ in the g2HDM. The upper limits on μ are calculated at 95% confidence level (CL) using a modified frequentist method [67–69] computed with an asymptotic approximation [70]. The expected 95% CL on the production cross section and the regions containing 68 and 95% of the distribution of the limits expected under the background-only hypothesis are calculated with pseudo-experiments using background-only samples. It is observed that the shapes of the BDT distributions are consistent with each other for different coupling values at the same A or H mass value. Therefore, for other coupling assumptions than ρtu/tc=0.4, the expected signal yields are scaled separately for ρtu and ρtc for each mass and coupling hypothesis making use of the corresponding signal cross sections. It is also observed that A or H can be used interchangeably as their corresponding BDT distribution shapes as well as their cross sections are the same. Therefore, we only show the results for A in this Letter. The observed and expected upper limits are displayed as functions of mA from 200 to 1000 GeV for ρtu=0.1,0.4,1.0 and ρtc=0.1,0.4,1.0, for the Run-2 data and for the combination of all three decay modes, without (with) A-H interference in Fig. 4(5). The observed limits at 95% CL on the signal strength as functions of mA and the new Yukawa couplings ρtc/tu are shown in Fig. 6 without A-H interference, and in Fig. 7 with A-H interference. Interpreted in g2HDM, exclusion limits at 95% CL on the mass of the additional Higgs bosons A and H are shown in Table 3 for different ρtu and ρtc assumptions.8SummaryA search for new Yukawa couplings of the top quark in models with additional Higgs bosons in proton-proton collisions at a center-of-mass energy of 13 TeV has been presented. The process considered is the production of same-sign top quark pairs associated with an up or a charm quark, and resulting in a final state containing two same-sign leptons and jets. No significant excess above the background prediction is observed. When no interference between the pseudoscalar (A) and scalar (H) Higgs bosons is assumed, A or H bosons with masses below 920 GeV and 1000 GeV are excluded at the 95% confidence level (CL) for coupling values ρtu=0.4 and 1.0, respectively, while all other extra Yukawa couplings are assumed to be zero. Similarly, without interference between H and A, and assuming a coupling value of ρtc=1.0, A or H bosons with masses below approximately 770GeV are excluded at the 95% CL. Under the assumption that A and H interfere in the scenario with a mass difference of mA−mH=50GeV, the pseudoscalar Higgs boson is excluded for mA values below 1000GeV when considering coupling values ρtu>0.4. Furthermore, assuming ρtc=0.4, the exclusion limit for A is mA=340GeV, whereas assuming ρtc=1.0, the limit extends to mA=810GeV at 95% CL. These results represent the first search based on the generalized two-Higgs-doublet model considering A-H interference.Declaration of Competing InterestThe authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.AcknowledgementsWe congratulate our colleagues in the CERN accelerator departments for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their contributions to the success of the CMS effort. In addition, we gratefully acknowledge the computing centers and personnel of the Worldwide LHC Computing Grid and other centers for delivering so effectively the computing infrastructure essential to our analyses. Finally, we acknowledge the enduring support for the construction and operation of the LHC, the CMS detector, and the supporting computing infrastructure provided by the following funding agencies: SC (Armenia), BMBWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, FAPERGS, and FAPESP (Brazil); MES and BNSF (Bulgaria); CERN; CAS, MOST, and NSFC (China); Minciencias (Colombia); MSES and CSF (Croatia); RIF (Cyprus); SENESCYT (Ecuador); MoER, ERC PUT and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); SRNSF (Georgia); BMBF, DFG, and HGF (Germany); GSRI (Greece); NKFIH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); MSIP and NRF (Republic of Korea); MES (Latvia); LAS (Lithuania); MOE and UM (Malaysia); BUAP, CINVESTAV, CONACYT, LNS, SEP, and UASLP-FAI (Mexico); MOS (Montenegro); MBIE (New Zealand); PAEC (Pakistan); MES and NSC (Poland); FCT (Portugal); MESTD (Serbia); MCIN/AEI and PCTI (Spain); MoSTR (Sri Lanka); Swiss Funding Agencies (Switzerland); MST (Taipei); MHESI and NSTDA (Thailand); TUBITAK and TENMAK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA).Individuals have received support from the Marie-Curie program and the European Research Council and Horizon 2020 Grant, contract Nos. 675440, 724704, 752730, 758316, 765710, 824093, and COST Action CA16108 (European Union); the Leventis Foundation; the Alfred P. Sloan Foundation; the Alexander von Humboldt Foundation; the Science Committee, project no. 22rl-037 (Armenia); the Belgian Federal Science Policy Office; the Fonds pour la Formation à la Recherche dans l'Industrie et dans l'Agriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); the F.R.S.-FNRS and FWO (Belgium) under the “Excellence of Science – EOS” – be.h project n. 30820817; the Beijing Municipal Science & Technology Commission, No. Z191100007219010 and Fundamental Research Funds for the Central Universities (China); The Ministry of Education, Youth and Sports (MEYS) of the Czech Republic; the Shota Rustaveli National Science Foundation, grant FR-22-985 (Georgia); the Deutsche Forschungsgemeinschaft (DFG), under Germany's Excellence Strategy – EXC 2121 “Quantum Universe” – 390833306, and under project number 400140256 - GRK2497; the Hellenic Foundation for Research and Innovation (HFRI), Project Number 2288 (Greece); the Hungarian Academy of Sciences, the New National Excellence Program - ÚNKP, the NKFIH research grants K 124845, K 124850, K 128713, K 128786, K 129058, K 131991, K 133046, K 138136, K 143460, K 143477, 2020-2.2.1-ED-2021-00181, and TKP2021-NKTA-64 (Hungary); the Council of Science and Industrial Research, India; ICSC – National Research Center for High Performance Computing, Big Data and Quantum Computing, funded by the EU NexGeneration program (Italy); the Latvian Council of Science; the Ministry of Education and Science, project no. 2022/WK/14, and the National Science Center, contracts Opus 2021/41/B/ST2/01369 and 2021/43/B/ST2/01552 (Poland); the Fundação para a Ciência e a Tecnologia, grant CEECIND/01334/2018 (Portugal); the National Priorities Research Program by Qatar National Research Fund; MCIN/AEI/10.13039/501100011033, ERDF “a way of making Europe”, and the Programa Estatal de Fomento de la Investigación Científica y Técnica de Excelencia María de Maeztu, grant MDM-2017-0765 and Programa Severo Ochoa del Principado de Asturias (Spain); the Chulalongkorn Academic into Its 2nd Century Project Advancement Project, and the National Science, Research and Innovation Fund via the Program Management Unit for Human Resources & Institutional Development, Research and Innovation, grant B05F650021 (Thailand); the Kavli Foundation; the Nvidia Corporation; the SuperMicro Corporation; the Welch Foundation, contract C-1845; and the Weston Havens Foundation (USA).References[1]ATLAS CollaborationObservation of a new particle in the search for the standard model Higgs boson with the ATLAS detector at the LHCPhys. 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SchnetzerS. SomalwarR. StoneS.A. ThayilS. ThomasJ. VoraH. WangH. AcharyaD. AllyA.G. DelannoyS. FiorendiS. HigginbothamT. HolmesA.R. KanugantiN. KarunarathnaL. LeeE. NibigiraS. SpanierD. AebiM. AhmadO. BouhaliM. DalchenkoR. EusebiJ. GilmoreT. HuangT. KamonH. KimS. LuoS. MalhotraR. MuellerD. OvertonD. RathjensA. SafonovN. AkchurinJ. DamgovV. HegdeA. HussainY. KazhykarimK. LamichhaneS.W. LeeA. MankelT. PeltolaI. VolobouevA. WhitbeckE. AppeltS. GreeneA. GurrolaW. JohnsR. Kunnawalkam ElayavalliA. MeloF. RomeoP. SheldonS. TuoJ. VelkovskaJ. ViinikainenB. CardwellB. CoxJ. HakalaR. HiroskyA. LedovskoyC. NeuC.E. Perez LaraP.E. KarchinA. AravindS. BanerjeeK. BlackT. BoseS. DasuI. De BruynP. EveraertsC. GalloniH. HeM. HerndonA. HerveC.K. KorakaA. LanaroR. LovelessJ. Madhusudanan SreekalaA. MallampalliA. MohammadiS. MondalG. ParidaD. PinnaA. SavinV. ShangV. SharmaW.H. SmithD. TeagueH.F. TsoiW. VetensA. WardenS. AfanasievV. AndreevYu. AndreevT. AushevM. AzarkinA. BabaevA. BelyaevV. BlinovE. BoosV. BorshchD. BudkouskiV. BunichevV. ChekhovskyR. ChistovM. DanilovA. DermenevT. DimovaD. DruzhkinM. DubininL. DudkoA. ErshovG. GavrilovV. GavrilovS. GninenkoV. GolovtcovN. GolubevI. GolutvinI. GorbunovA. GribushinY. IvanovV. KachanovV. KarjavineA. KarneyeuV. KimM. KirakosyanD. KirpichnikovM. KirsanovV. KlyukhinV. KorenkovA. KozyrevN. KrasnikovA. LanevP. LevchenkoN. LychkovskayaV. MakarenkoA. MalakhovV. MatveevV. MurzinA. NikitenkoS. ObraztsovV. OreshkinV. PalichikV. PerelyginM. PerfilovS. PolikarpovV. PopovO. RadchenkoM. SavinaV. SavrinV. ShalaevS. ShmatovS. ShulhaY. SkovpenS. SlabospitskiiV. SmirnovD. SosnovV. SulimovE. TcherniaevA. TerkulovO. TeryaevI. TlisovaA. ToropinL. UvarovA. UzunianP. VolkovA. VorobyevG. VorotnikovN. VoytishinB.S. YuldashevA. ZarubinI. ZhizhinA. ZhokinCMSTop quarksExtra Higgs bosonYukawa couplingsPhysics Letters B 850 (2024). doi:10.1016/j.physletb.2024.138478journalPhysics Letters B© 2024 The Author(s). Published by Elsevier B.V. Funded by SCOAP³.Elsevier B.V.0370-2693850March 202410.1016/j.physletb.2024.138478http://dx.doi.org/10.1016/j.physletb.2024.138478doi:10.1016/j.physletb.2024.138478138478http://vtw.elsevier.com/data/voc/oa/OpenAccessStatus#Full2024-01-12T00:06:30ZSCOAP³ - Sponsoring Consortium for Open Access Publishing in Particle Physicshttp://vtw.elsevier.com/data/voc/oa/SponsorType#FundingBodyhttp://creativecommons.org/licenses/by/4.0/2024-02-02T00:00:00.000Z2024-02-09T00:00:00.000ZThis is an open access article under the CC BY license.JournalsS300.3PLB138478138478S0370-2693(24)00017-010.1016/j.physletb.2024.138478The Author(s)ExperimentsCMSdata preservation, re-use and open access policyFig. 1Representative Feynman diagram for ttq‾ (q = u, c) production through a new scalar (H) or pseudoscalar (A) Higgs boson. In this analysis, events with q = q′ are considered.Fig. 1Fig. 2The pre-fit CvsL (upper) and CvsB (lower) distributions for the selected highest pT jet. The predictions for mA = 350 GeV with A-H interference assuming mA − mH = 50 GeV for ρtu = 1.0 (solid red line) and ρtc = 1.0 (dashed red line) are also displayed. The numbers in square brackets represent the yields for each sample. The uncertainty bars on the points and the hatched bands represent the statistical uncertainties in the data and in the background predictions, respectively. Beneath each plot the ratio of data to predictions is shown. The uncertainty bars in the ratio plots include statistical uncertainties in the data and in the background predictions.Fig. 2Fig. 3Post-fit distributions of the BDT discriminants combining the categories e±e±, μ±μ±, and e±μ±, and all data-taking periods, for mA = 350 GeV with ρtu = 1.0 (upper), and ρtc = 1.0 (lower) with the A-H interference. The numbers in square brackets represent the yields for each sample. The uncertainty bars on the points represent the statistical uncertainties in the data. Beneath each plot the ratio of data to predictions is shown. The uncertainty bars in the ratio plots include statistical uncertainties in the data and the total uncertainty in the background predictions, and the hatched bands represent the total uncertainty in the background predictions.Fig. 3Fig. 4Observed and expected 95% CL upper limits on the signal strength as functions of mA for g2HDM using different coupling assumptions: ρtu = 0.1, 0.4, 1.0 (upper) and ρtc = 0.1, 0.4, 1.0 (lower) without interference, for the combination of the e±e±, μ±μ±, and e±μ± categories and all data-taking periods. The inner (green) band and the outer (yellow) band indicate the regions containing 68 and 95%, respectively, of the distribution of limits expected under the background-only hypothesis.Fig. 4Fig. 5Observed and expected 95% CL upper limits on the signal strength as functions of mA for g2HDM using different coupling assumptions: ρtu = 0.1, 0.4, 1.0 (upper) and ρtc = 0.1, 0.4, 1.0 (lower) with A-H interference assuming mA − mH = 50 GeV, for the combination of the e±e±, μ±μ±, and e±μ± categories and all data-taking periods. The inner (green) band and the outer (yellow) band indicate the regions containing 68 and 95%, respectively, of the distribution of limits expected under the background-only hypothesis.Fig. 5Fig. 6Observed 95% CL upper limit on the signal strength as a function of mA and ρtu (upper) and ρtc (lower) for g2HDM without the A-H interference, for the combination of the e±e±, μ±μ±, and e±μ± categories. The color axis represents the observed upper limit on the signal strength. Expected (dashed lines) and observed (solid lines) exclusion contours are also shown.Fig. 6Fig. 7Observed 95% CL upper limit on the signal strength as a function of mA and ρtu (upper) and ρtc (lower) for g2HDM signal model with the A-H interference, for the combination of the e±e±, μ±μ±, and e±μ± categories. The color axis represents the observed upper limit on the signal strength. Expected (dashed lines) and observed (solid lines) exclusion contours are also shown.Fig. 7Table 1Input variables of the BDT. Jets and leptons are ordered by pT.Table 1Input variables of the BDTCvsL(ja)a = 1,2,3Charm- vs light-quark jet identification variableCvsB(ja)a = 1,2,3Charm- vs bottom-quark jet identification variableΔR(ja,jb)1 ≤ a < b ≤ 3Angular separation between jetsm(ja,jb)1 ≤ a < b ≤ 3Invariant mass of jet pairsΔR(ja,lb)a = 1,2,3; b = 1,2Angular separation between jet and leptonm(ja,lb)a = 1,2,3; b = 1,2Invariant mass of jet-lepton pairspT(ℓa)a = 1,2Transverse momentum of leptonsm(ℓ1,ℓ2,ja)a = 1,2,3Invariant mass of the two leptons plus the highest pT jetm(ℓ1,ℓ2)Invariant mass of the two leptonsHTScalar pT sum of the jetspTmissMissing transverse momentumTable 2Summary of systematic uncertainties for ρtc = 0.4 and mA = 350 GeV with A-H interference assuming mA − mH = 50 GeV. The first column indicates the source of uncertainty. The second column specifies whether the shape of the fit discriminant is affected by the nuisance parameter (✓) or not (dash). The impact in percent of these nuisance parameters on the pre-fit expected event yields is displayed in the third column. This column is subdivided into three event categories representing the analysis channels. The percentage impacts are given as a range of values representing the minimum and maximum differences obtained in the different bins of the BDT distribution through the four data-taking periods. The numbers for the normalization component of the nonprompt lepton background represent the uncertainties used for each data-taking period. Whether or not a nuisance parameter is taken correlated across years and categories is specified in the last two columns. The luminosity and jet flavor identification nuisances are only partially correlated across years.Table 2Uncertainty sourceShapeCategoryCorrelated acrosse±e±μ±μ±e±μ±YearsCategoriesExperimentalLuminosity—1.2–2.51.2–2.51.2–2.5✓✓Pileup✓<0.1–2.8<0.1–1.8<0.1–2.3✓✓Trigger efficiency✓0.4–2.60.2–1.10.3–1.2——L1 trigger inefficiency✓0.1–0.80.1–0.30.1–0.4✓✓Lepton identification✓0.1–1.7<0.1–0.4<0.1–0.6—✓Lepton energy scale✓—<0.1–0.2<0.1–0.2—✓Charge misid.✓1.2–13.1————Jet energy scale✓<0.1–4.5<0.1–1.7<0.1–1.5✓✓Jet energy resolution✓<0.1–2.6<0.1–1.8<0.1–1.6—✓Unclustered energy✓<0.1–2.6<0.1–0.5<0.1–0.8—✓Jet flavor identification✓<0.1–12.1<0.1–8.8<0.1–11.6✓✓Nonprompt lepton BGstatistical component✓<0.1–27.21.9–16.23.0–13.2—✓Nonprompt lepton BG—27,15,11,1027,15,11,1027,15,11,10—✓TheoreticalSignal QCD scales✓10.3–10.510.0–10.29.9–10.0✓✓Signal PDF✓0.70.6–0.70.5–0.6✓✓Signal parton shower✓3.6–4.34.0–4.36.3–7.3✓✓tt‾—6.16.16.1✓✓VV—4.54.54.5✓✓VBS—10.410.410.4✓✓tt‾H—7.87.87.8✓✓tt‾W—10.710.710.7✓✓Other backgrounds—5.45.45.4✓✓Table 3Observed (expected) lower limits on mA at 95% CL. For the scenario without interference, the limits on mH and mA are the same.Table 3Observed (expected) mass limit [GeV]withoutwithwithinterferenceinterferenceinterferencemA or mHmAmHρtu0.4920 (920)1000 (1000)950 (950)1.01000 (1000)1000 (1000)950 (950)ρtc0.4no limit340 (370)290 (320)1.0770 (680)810 (670)760 (620)LetterSearch for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at s=13TeVThe CMS Collaboration⋆A.HayrapetyanA.Tumasyan1Yerevan Physics Institute, Yerevan, ArmeniaYerevan Physics InstituteYerevanArmeniaYerevan Physics Institute, Yerevan, Armenia1Also at Yerevan State University, Yerevan, Armenia.W.AdamJ.W.AndrejkovicT.BergauerS.ChatterjeeK.DamanakisM.DragicevicP.S.HussainM.Jeitler2N.KrammerA.LiD.LikoI.MikulecJ.Schieck2R.SchöfbeckD.SchwarzM.SonawaneS.TemplW.WaltenbergerC.-E.Wulz2Institut für Hochenergiephysik, Vienna, AustriaInstitut für HochenergiephysikViennaAustriaInstitut für Hochenergiephysik, Vienna, Austria2Also at TU Wien, Vienna, Austria.M.R.Darwish3T.JanssenP.Van MechelenUniversiteit Antwerpen, Antwerpen, BelgiumUniversiteit AntwerpenAntwerpenBelgiumUniversiteit Antwerpen, Antwerpen, Belgium3Also at Institute of Basic and Applied Sciences, Faculty of Engineering, Arab Academy for Science, Technology and Maritime Transport, Alexandria, Egypt.E.S.BolsJ.D'HondtS.DansanaA.De MoorM.DelcourtH.El FahamS.LowetteI.MakarenkoD.MüllerA.R.SahasransuS.TavernierM.Tytgat4S.Van PutteD.VanneromVrije Universiteit Brussel, Brussel, BelgiumVrije Universiteit BrusselBrusselBelgiumVrije Universiteit Brussel, Brussel, Belgium4Also at Ghent University, Ghent, Belgium.B.ClerbauxG.De LentdeckerL.FavartD.HohovJ.JaramilloA.KhalilzadehK.LeeM.MahdavikhorramiA.MalaraS.ParedesL.PétréN.PostiauL.ThomasM.Vanden BemdenC.Vander VeldeP.VanlaerUniversité Libre de Bruxelles, Bruxelles, BelgiumUniversité Libre de BruxellesBruxellesBelgiumUniversité Libre de Bruxelles, Bruxelles, BelgiumM.De CoenD.DoburY.HongJ.KnolleL.LambrechtG.MestdachC.RendónA.SamalanK.SkovpenN.Van Den BosscheJ.van der LindenL.WezenbeekGhent University, Ghent, BelgiumGhent UniversityGhentBelgiumGhent University, Ghent, BelgiumA.BeneckeG.BrunoC.CaputoC.DelaereI.S.DonertasA.GiammancoK.JaffelSa.JainV.LemaitreJ.LidrychP.MastrapasquaK.MondalT.T.TranS.WertzUniversité Catholique de Louvain, Louvain-la-Neuve, BelgiumUniversité Catholique de LouvainLouvain-la-NeuveBelgiumUniversité Catholique de Louvain, Louvain-la-Neuve, BelgiumG.A.AlvesE.CoelhoC.HenselT.Menezes De OliveiraA.MoraesP.Rebello TelesM.SoeiroCentro Brasileiro de Pesquisas Fisicas, Rio de Janeiro, BrazilCentro Brasileiro de Pesquisas FisicasRio de JaneiroBrazilCentro Brasileiro de Pesquisas Fisicas, Rio de Janeiro, BrazilW.L.Aldá JúniorM.Alves Gallo PereiraM.Barroso Ferreira FilhoH.Brandao MalbouissonW.CarvalhoJ.Chinellato5E.M.Da CostaG.G.Da Silveira6D.De Jesus DamiaoS.Fonseca De SouzaJ.Martins7C.Mora HerreraK.Mota AmariloL.MundimH.NogimaA.SantoroA.SznajderM.ThielA.Vilela PereiraUniversidade do Estado do Rio de Janeiro, Rio de Janeiro, BrazilUniversidade do Estado do Rio de JaneiroRio de JaneiroBrazilUniversidade do Estado do Rio de Janeiro, Rio de Janeiro, Brazil5Also at Universidade Estadual de Campinas, Campinas, Brazil.6Also at Federal University of Rio Grande do Sul, Porto Alegre, Brazil.7Also at UFMS, Nova Andradina, Brazil.C.A.Bernardes6L.CalligarisT.R.Fernandez Perez TomeiE.M.GregoresP.G.MercadanteS.F.NovaesB.OrzariSandra S.PadulaUniversidade Estadual Paulista, Universidade Federal do ABC, São Paulo, BrazilUniversidade Estadual PaulistaUniversidade Federal do ABCSão PauloBrazilUniversidade Estadual Paulista, Universidade Federal do ABC, São Paulo, BrazilA.AleksandrovG.AntchevR.HadjiiskaP.IaydjievM.MishevaM.ShopovaG.SultanovInstitute for Nuclear Research and Nuclear Energy, Bulgarian Academy of Sciences, Sofia, BulgariaInstitute for Nuclear Research and Nuclear EnergyBulgarian Academy of SciencesSofiaBulgariaInstitute for Nuclear Research and Nuclear Energy, Bulgarian Academy of Sciences, Sofia, BulgariaA.DimitrovL.LitovB.PavlovP.PetkovA.PetrovE.ShumkaUniversity of Sofia, Sofia, BulgariaUniversity of SofiaSofiaBulgariaUniversity of Sofia, Sofia, BulgariaS.KeshriS.ThakurInstituto De Alta Investigación, Universidad de Tarapacá, Casilla 7 D, Arica, ChileInstituto De Alta InvestigaciónUniversidad de TarapacáCasilla 7 DAricaChileInstituto De Alta Investigación, Universidad de Tarapacá, Casilla 7 D, Arica, ChileT.ChengQ.GuoT.JavaidL.YuanBeihang University, Beijing, ChinaBeihang UniversityBeijingChinaBeihang University, Beijing, ChinaZ.HuJ.LiuK.Yi89Department of Physics, Tsinghua University, Beijing, ChinaDepartment of PhysicsTsinghua UniversityBeijingChinaDepartment of Physics, Tsinghua University, Beijing, China8Also at Nanjing Normal University, Nanjing, China.9Now at The University of Iowa, Iowa City, Iowa, USA.G.M.Chen10H.S.Chen10M.Chen10F.IemmiC.H.JiangA.Kapoor11H.LiaoZ.-A.Liu12R.Sharma13J.N.Song12J.TaoC.Wang10J.WangZ.Wang10H.ZhangInstitute of High Energy Physics, Beijing, ChinaInstitute of High Energy PhysicsBeijingChinaInstitute of High Energy Physics, Beijing, China10Also at University of Chinese Academy of Sciences, Beijing, China.11Also at China Center of Advanced Science and Technology, Beijing, China.12Also at University of Chinese Academy of Sciences, Beijing, China.13Also at China Spallation Neutron Source, Guangdong, China.A.AgapitosY.BanA.LevinC.LiQ.LiY.MaoS.J.QianX.SunD.WangH.YangL.ZhangC.ZhouState Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, ChinaState Key Laboratory of Nuclear Physics and TechnologyPeking UniversityBeijingChinaState Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, ChinaZ.YouSun Yat-Sen University, Guangzhou, ChinaSun Yat-Sen UniversityGuangzhouChinaSun Yat-Sen University, Guangzhou, ChinaN.LuUniversity of Science and Technology of China, Hefei, ChinaUniversity of Science and Technology of ChinaHefeiChinaUniversity of Science and Technology of China, Hefei, ChinaG.Bauer14Nanjing Normal University, Nanjing, ChinaNanjing Normal UniversityNanjingChinaNanjing Normal University, Nanjing, China14Now at Henan Normal University, Xinxiang, China.X.Gao15D.LeggatH.OkawaY.ZhangInstitute of Modern Physics and Key Laboratory of Nuclear Physics and Ion-beam Application (MOE) - Fudan University, Shanghai, ChinaInstitute of Modern PhysicsKey Laboratory of Nuclear PhysicsIon-beam Application (MOE)Fudan UniversityShanghaiChinaInstitute of Modern Physics and Key Laboratory of Nuclear Physics and Ion-beam Application (MOE) - Fudan University, Shanghai, China15Also at Université Libre de Bruxelles, Bruxelles, Belgium.Z.LinC.LuM.XiaoZhejiang University, Hangzhou, Zhejiang, ChinaZhejiang UniversityHangzhouZhejiangChinaZhejiang University, Hangzhou, Zhejiang, ChinaC.AvilaD.A.Barbosa TrujilloA.CabreraC.FlorezJ.FragaJ.A.Reyes VegaUniversidad de Los Andes, Bogota, ColombiaUniversidad de Los AndesBogotaColombiaUniversidad de Los Andes, Bogota, ColombiaJ.Mejia GuisaoF.RamirezM.RodriguezJ.D.Ruiz AlvarezUniversidad de Antioquia, Medellin, ColombiaUniversidad de AntioquiaMedellinColombiaUniversidad de Antioquia, Medellin, ColombiaD.GiljanovicN.GodinovicD.LelasA.SculacUniversity of Split, Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, Split, CroatiaUniversity of SplitFaculty of Electrical Engineering, Mechanical Engineering and Naval ArchitectureSplitCroatiaUniversity of Split, Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, Split, CroatiaM.KovacT.Sculac16University of Split, Faculty of Science, Split, CroatiaUniversity of SplitFaculty of ScienceSplitCroatiaUniversity of Split, Faculty of Science, Split, Croatia16Also at University of Latvia (LU), Riga, Latvia.P.BargassaV.BrigljevicB.K.ChitrodaD.FerencekS.MishraA.Starodumov17T.SusaInstitute Rudjer Boskovic, Zagreb, CroatiaInstitute Rudjer BoskovicZagrebCroatiaInstitute Rudjer Boskovic, Zagreb, Croatia17Also at an institute or an international laboratory covered by a cooperation agreement with CERN.A.AttikisK.ChristoforouS.KonstantinouJ.MousaC.NicolaouF.PtochosP.A.RazisH.RykaczewskiH.SakaA.StepennovUniversity of Cyprus, Nicosia, CyprusUniversity of CyprusNicosiaCyprusUniversity of Cyprus, Nicosia, CyprusM.FingerM.FingerJr.A.KvetonCharles University, Prague, Czech RepublicCharles UniversityPragueCzech RepublicCharles University, Prague, Czech RepublicE.AyalaEscuela Politecnica Nacional, Quito, EcuadorEscuela Politecnica NacionalQuitoEcuadorEscuela Politecnica Nacional, Quito, EcuadorE.Carrera JarrinUniversidad San Francisco de Quito, Quito, EcuadorUniversidad San Francisco de QuitoQuitoEcuadorUniversidad San Francisco de Quito, Quito, EcuadorH.Abdalla18Y.Assran1920Academy of Scientific Research and Technology of the Arab Republic of Egypt, Egyptian Network of High Energy Physics, Cairo, EgyptAcademy of Scientific Research and Technology of the Arab Republic of EgyptEgyptian Network of High Energy PhysicsCairoEgyptAcademy of Scientific Research and Technology of the Arab Republic of Egypt, Egyptian Network of High Energy Physics, Cairo, Egypt18Also at Cairo University, Cairo, Egypt.19Also at Suez University, Suez, Egypt.20Now at British University in Egypt, Cairo, Egypt.M.A.MahmoudY.MohammedCenter for High Energy Physics (CHEP-FU), Fayoum University, El-Fayoum, EgyptCenter for High Energy Physics (CHEP-FU)Fayoum UniversityEl-FayoumEgyptCenter for High Energy Physics (CHEP-FU), Fayoum University, El-Fayoum, EgyptR.K.Dewanjee21K.EhatahtM.KadastikT.LangeS.NandanC.NielsenJ.PataM.RaidalL.TaniC.VeelkenNational Institute of Chemical Physics and Biophysics, Tallinn, EstoniaNational Institute of Chemical Physics and BiophysicsTallinnEstoniaNational Institute of Chemical Physics and Biophysics, Tallinn, Estonia21Also at Birla Institute of Technology, Mesra, Mesra, India.H.KirschenmannK.OsterbergM.VoutilainenDepartment of Physics, University of Helsinki, Helsinki, FinlandDepartment of PhysicsUniversity of HelsinkiHelsinkiFinlandDepartment of Physics, University of Helsinki, Helsinki, FinlandS.BharthuarE.BrückenF.GarciaJ.HavukainenK.T.S.KallonenR.KinnunenT.LampénK.Lassila-PeriniS.LehtiT.LindénM.LottiL.MartikainenM.MyllymäkiM.m.RantanenH.SiikonenE.TuominenJ.TuominiemiHelsinki Institute of Physics, Helsinki, FinlandHelsinki Institute of PhysicsHelsinkiFinlandHelsinki Institute of Physics, Helsinki, FinlandP.LuukkaH.PetrowT.Tuuva†Lappeenranta-Lahti University of Technology, Lappeenranta, FinlandLappeenranta-Lahti University of TechnologyLappeenrantaFinlandLappeenranta-Lahti University of Technology, Lappeenranta, Finland†Deceased.M.BesanconF.CoudercM.DejardinD.DenegriJ.L.FaureF.FerriS.GanjourP.GrasG.Hamel de MonchenaultV.LohezicJ.MalclesJ.RanderA.RosowskyM.Ö.SahinA.Savoy-Navarro22P.SimkinaM.TitovM.TornagoIRFU, CEA, Université Paris-Saclay, Gif-sur-Yvette, FranceIRFUCEAUniversité Paris-SaclayGif-sur-YvetteFranceIRFU, CEA, Université Paris-Saclay, Gif-sur-Yvette, France22Also at Purdue University, West Lafayette, Indiana, USA.C.Baldenegro BarreraF.BeaudetteA.Buchot PerraguinP.BussonA.CappatiC.CharlotF.DamasO.DavignonA.De WitG.FalmagneB.A.Fontana Santos AlvesS.GhoshA.GilbertR.Granier de CassagnacA.HakimiB.HarikrishnanL.KalipolitiG.LiuJ.MottaM.NguyenC.OchandoL.PortalesR.SalernoJ.B.SauvanY.SiroisA.TarabiniE.VernazzaA.ZabiA.ZghicheLaboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, FranceLaboratoire Leprince-RinguetCNRS/IN2P3Ecole PolytechniqueInstitut Polytechnique de ParisPalaiseauFranceLaboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, FranceJ.-L.Agram23J.AndreaD.ApparuD.BlochJ.-M.BromE.C.ChabertC.CollardS.FalkeU.GoerlachC.GrimaultR.HaeberleA.-C.Le BihanM.MeenaG.SahaM.A.SessiniP.Van HoveUniversité de Strasbourg, CNRS, IPHC UMR 7178, Strasbourg, FranceUniversité de StrasbourgCNRSIPHC UMR 7178StrasbourgFranceUniversité de Strasbourg, CNRS, IPHC UMR 7178, Strasbourg, France23Also at Université de Haute Alsace, Mulhouse, France.S.BeauceronB.BlanconG.BoudoulN.ChanonJ.ChoiD.ContardoP.DepasseC.Dozen24H.El MamouniJ.FayS.GasconM.GouzevitchC.GreenbergG.GrenierB.IlleI.B.LaktinehM.LethuillierL.MirabitoS.PerriesA.PurohitM.Vander DoncktP.VerdierJ.XiaoInstitut de Physique des 2 Infinis de Lyon (IP2I), Villeurbanne, FranceInstitut de Physique des 2 Infinis de Lyon (IP2I)VilleurbanneFranceInstitut de Physique des 2 Infinis de Lyon (IP2I ), Villeurbanne, France24Also at Department of Physics, Tsinghua University, Beijing, China.A.Khvedelidze17I.LomidzeZ.Tsamalaidze17Georgian Technical University, Tbilisi, GeorgiaGeorgian Technical UniversityTbilisiGeorgiaGeorgian Technical University, Tbilisi, GeorgiaV.BottaL.FeldK.KleinM.LipinskiD.MeuserA.PaulsN.RöwertM.TeroerdeRWTH Aachen University, I. Physikalisches Institut, Aachen, GermanyRWTH Aachen UniversityI. Physikalisches InstitutAachenGermanyRWTH Aachen University, I. Physikalisches Institut, Aachen, GermanyS.DiekmannA.DodonovaN.EichD.EliseevF.EngelkeM.ErdmannP.FackeldeyB.FischerT.HebbekerK.HoepfnerF.IvoneA.JungM.y.LeeL.MastrolorenzoF.MausolfM.MerschmeyerA.MeyerS.MukherjeeD.NollA.NovakF.NowotnyA.PozdnyakovY.RathW.RedjebF.RehmH.ReithlerU.SarkarV.SarkisoviA.SchmidtA.SharmaJ.L.SpahA.SteinF.Torres Da Silva De Araujo25L.VigilanteS.WiedenbeckS.ZaleskiRWTH Aachen University, III. Physikalisches Institut A, Aachen, GermanyRWTH Aachen UniversityIII. Physikalisches Institut AAachenGermanyRWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany25Also at The University of the State of Amazonas, Manaus, Brazil.C.DziwokG.FlüggeW.Haj Ahmad26T.KressA.NowackO.PoothA.StahlT.ZiemonsA.ZotzRWTH Aachen University, III. Physikalisches Institut B, Aachen, GermanyRWTH Aachen UniversityIII. Physikalisches Institut BAachenGermanyRWTH Aachen University, III. Physikalisches Institut B, Aachen, Germany26Also at Erzincan Binali Yildirim University, Erzincan, Turkey.H.Aarup PetersenM.Aldaya MartinJ.AlimenaS.AmorosoY.AnS.BaxterM.BayatmakouH.Becerril GonzalezO.BehnkeA.BelvedereS.BhattacharyaF.Blekman27K.Borras28D.BrunnerA.CampbellA.CardiniC.ChengF.ColombinaS.Consuegra RodríguezG.Correia SilvaM.De SilvaG.EckerlinD.EcksteinL.I.Estevez BanosO.FilatovE.Gallo27A.GeiserA.GiraldiG.GreauV.GuglielmiM.GuthoffA.HinzmannA.Jafari29L.JeppeN.Z.JomhariB.KaechM.KasemannH.KavehC.KleinwortR.KoglerM.KommD.KrückerW.LangeD.Leyva PerniaK.Lipka30W.Lohmann31R.MankelI.-A.Melzer-PellmannM.Mendizabal MorentinJ.MetwallyA.B.MeyerG.MilellaA.MussgillerL.P.NairA.NürnbergY.OtaridJ.ParkD.Pérez AdánE.RankenA.RasperezaB.Ribeiro LopesJ.RübenachA.SaggioM.Scham3228S.Schnake28P.SchützeC.Schwanenberger27D.SelivanovaM.ShchedrolosievR.E.Sosa RicardoD.StaffordF.VazzolerA.Ventura BarrosoR.WalshQ.WangY.WenK.WichmannL.Wiens28C.WissingY.YangA.Zimermmane Castro SantosDeutsches Elektronen-Synchrotron, Hamburg, GermanyDeutsches Elektronen-SynchrotronHamburgGermanyDeutsches Elektronen-Synchrotron, Hamburg, Germany27Also at University of Hamburg, Hamburg, Germany.28Also at RWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany.29Also at Isfahan University of Technology, Isfahan, Iran.30Also at Bergische University Wuppertal (BUW), Wuppertal, Germany.31Also at Brandenburg University of Technology, Cottbus, Germany.32Also at Forschungszentrum Jülich, Juelich, Germany.A.AlbrechtS.AlbrechtM.AntonelloS.BeinL.BenatoM.BonanomiP.ConnorM.EichK.El MorabitY.FischerA.FröhlichC.GarbersE.GaruttiA.GrohsjeanM.HajheidariJ.HallerH.R.JabuschG.KasieczkaP.KeicherR.KlannerW.KorcariT.KramerV.KutznerF.LabeJ.LangeA.LobanovC.MatthiesA.MehtaL.MoureauxM.MrowietzA.NigamovaY.NissanA.PaaschK.J.Pena RodriguezT.QuadfaselB.RacitiM.RiegerD.SavoiuJ.SchindlerP.SchleperM.SchröderJ.SchwandtM.SommerhalderH.StadieG.SteinbrückA.TewsM.WolfUniversity of Hamburg, Hamburg, GermanyUniversity of HamburgHamburgGermanyUniversity of Hamburg, Hamburg, GermanyS.BrommerM.BurkartE.ButzT.ChwalekA.DierlammA.DrollN.FaltermannM.GiffelsA.GottmannF.Hartmann33R.HofsaessM.HorzelaU.HusemannJ.KieselerM.KluteR.KoppenhöferJ.M.LawhornM.LinkA.LintuluotoS.MaierS.MitraM.MormileTh.MüllerM.NeukumM.OhM.PresillaG.QuastK.RabbertzB.RegneryN.ShadskiyI.ShvetsovH.J.SimonisM.Toms34N.TrevisaniR.UlrichR.F.Von CubeM.WassmerS.WielandF.WittigR.WolfS.WunschX.ZuoKarlsruher Institut fuer Technologie, Karlsruhe, GermanyKarlsruher Institut fuer TechnologieKarlsruheGermanyKarlsruher Institut fuer Technologie, Karlsruhe, Germany33Also at CERN, European Organization for Nuclear Research, Geneva, Switzerland.34Now at an institute or an international laboratory covered by a cooperation agreement with CERN.G.AnagnostouG.DaskalakisA.KyriakisA.Papadopoulos33A.StakiaInstitute of Nuclear and Particle Physics (INPP), NCSR Demokritos, Aghia Paraskevi, GreeceInstitute of Nuclear and Particle Physics (INPP)NCSR DemokritosAghia ParaskeviGreeceInstitute of Nuclear and Particle Physics (INPP), NCSR Demokritos, Aghia Paraskevi, GreeceP.KontaxakisG.MelachroinosA.PanagiotouI.PapavergouI.ParaskevasN.SaoulidouK.TheofilatosE.TziaferiK.VellidisI.ZisopoulosNational and Kapodistrian University of Athens, Athens, GreeceNational and Kapodistrian University of AthensAthensGreeceNational and Kapodistrian University of Athens, Athens, GreeceG.BakasT.ChatzistavrouG.KarapostoliK.KousourisI.PapakrivopoulosE.SiamarkouG.TsipolitisA.ZacharopoulouNational Technical University of Athens, Athens, GreeceNational Technical University of AthensAthensGreeceNational Technical University of Athens, Athens, GreeceK.AdamidisI.BestintzanosI.EvangelouC.FoudasP.GianneiosC.KamtsikisP.KatsoulisP.KokkasP.G.Kosmoglou KioseoglouN.ManthosI.PapadopoulosJ.StrologasUniversity of Ioánnina, Ioánnina, GreeceUniversity of IoánninaIoánninaGreeceUniversity of Ioánnina, Ioánnina, GreeceM.Bartók35C.HajduD.Horvath3637F.SiklerV.VeszpremiHUN-REN Wigner Research Centre for Physics, Budapest, HungaryHUN-REN Wigner Research Centre for PhysicsBudapestHungaryHUN-REN Wigner Research Centre for Physics, Budapest, Hungary35Also at Institute of Physics, University of Debrecen, Debrecen, Hungary.36Also at Institute of Nuclear Research ATOMKI, Debrecen, Hungary.37Now at Universitatea Babes-Bolyai - Facultatea de Fizica, Cluj-Napoca, Romania.M.CsanádK.FarkasM.M.A.Gadallah38Á.KadlecsikP.MajorK.MandalG.PásztorA.J.Rádl39G.I.VeresMTA-ELTE Lendület CMS Particle and Nuclear Physics Group, Eötvös Loránd University, Budapest, HungaryMTA-ELTE Lendület CMS Particle and Nuclear Physics GroupEötvös Loránd UniversityBudapestHungaryMTA-ELTE Lendület CMS Particle and Nuclear Physics Group, Eötvös Loránd University, Budapest, Hungary38Also at Physics Department, Faculty of Science, Assiut University, Assiut, Egypt.39Also at HUN-REN Wigner Research Centre for Physics, Budapest, Hungary.P.RaicsB.UjvariG.ZiliziFaculty of Informatics, University of Debrecen, Debrecen, HungaryFaculty of InformaticsUniversity of DebrecenDebrecenHungaryFaculty of Informatics, University of Debrecen, Debrecen, HungaryG.BenczeS.CzellarJ.Karancsi35J.MolnarZ.SzillasiInstitute of Nuclear Research ATOMKI, Debrecen, HungaryInstitute of Nuclear Research ATOMKIDebrecenHungaryInstitute of Nuclear Research ATOMKI, Debrecen, HungaryT.Csorgo39F.Nemes39T.NovakKaroly Robert Campus, MATE Institute of Technology, Gyongyos, HungaryMATE Institute of TechnologyKaroly Robert CampusGyongyosHungaryKaroly Robert Campus, MATE Institute of Technology, Gyongyos, HungaryJ.BabbarS.BansalS.B.BeriV.BhatnagarG.ChaudharyS.ChauhanN.Dhingra40A.KaurA.KaurH.KaurM.KaurS.KumarK.SandeepT.SheokandJ.B.SinghA.SinglaPanjab University, Chandigarh, IndiaPanjab UniversityChandigarhIndiaPanjab University, Chandigarh, India40Also at Punjab Agricultural University, Ludhiana, India.A.AhmedA.BhardwajA.ChhetriB.C.ChoudharyA.KumarA.KumarM.NaimuddinK.RanjanS.SaumyaUniversity of Delhi, Delhi, IndiaUniversity of DelhiDelhiIndiaUniversity of Delhi, Delhi, IndiaS.BaradiaS.Barman41S.BhattacharyaS.DuttaS.DuttaP.PalitS.SarkarSaha Institute of Nuclear Physics, HBNI, Kolkata, IndiaSaha Institute of Nuclear PhysicsHBNIKolkataIndiaSaha Institute of Nuclear Physics, HBNI, Kolkata, India41Also at University of Visva-Bharati, Santiniketan, India.M.M.AmeenP.K.BeheraS.C.BeheraS.ChatterjeeP.JanaP.KalbhorJ.R.Komaragiri42D.Kumar42L.Panwar42P.R.PujahariN.R.SahaA.SharmaA.K.SikdarS.VermaIndian Institute of Technology Madras, Madras, IndiaIndian Institute of Technology MadrasMadrasIndiaIndian Institute of Technology Madras, Madras, India42Also at Indian Institute of Science (IISc), Bangalore, India.S.DugadM.KumarG.B.MohantyP.SuryadevaraTata Institute of Fundamental Research-A, Mumbai, IndiaTata Institute of Fundamental Research-AMumbaiIndiaTata Institute of Fundamental Research-A, Mumbai, IndiaA.BalaS.BanerjeeR.M.ChatterjeeM.GuchaitSh.JainS.KarmakarS.KumarG.MajumderK.MazumdarS.ParoliaA.ThachayathTata Institute of Fundamental Research-B, Mumbai, IndiaTata Institute of Fundamental Research-BMumbaiIndiaTata Institute of Fundamental Research-B, Mumbai, IndiaS.Bahinipati43A.K.DasC.KarD.Maity44P.MalT.MishraV.K.Muraleedharan Nair Bindhu44K.Naskar44A.Nayak44P.SadangiP.SahaS.K.SwainS.Varghese44D.Vats44National Institute of Science Education and Research, An OCC of Homi Bhabha National Institute, Bhubaneswar, Odisha, IndiaNational Institute of Science Education and ResearchAn OCC of Homi Bhabha National InstituteBhubaneswarOdishaIndiaNational Institute of Science Education and Research, An OCC of Homi Bhabha National Institute, Bhubaneswar, Odisha, India43Also at IIT Bhubaneswar, Bhubaneswar, India.44Also at Institute of Physics, Bhubaneswar, India.S.Acharya45A.AlpanaS.DubeB.Gomber45B.KansalA.LahaB.Sahu45S.SharmaIndian Institute of Science Education and Research (IISER), Pune, IndiaIndian Institute of Science Education and Research (IISER)PuneIndiaIndian Institute of Science Education and Research (IISER), Pune, India45Also at University of Hyderabad, Hyderabad, India.H.Bakhshiansohi46E.Khazaie47M.Zeinali48Isfahan University of Technology, Isfahan, IranIsfahan University of TechnologyIsfahanIranIsfahan University of Technology, Isfahan, Iran46Also at Deutsches Elektronen-Synchrotron, Hamburg, Germany.47Also at Department of Physics, Isfahan University of Technology, Isfahan, Iran.48Also at Sharif University of Technology, Tehran, Iran.S.Chenarani49S.M.EtesamiM.KhakzadM.Mohammadi NajafabadiInstitute for Research in Fundamental Sciences (IPM), Tehran, IranInstitute for Research in Fundamental Sciences (IPM)TehranIranInstitute for Research in Fundamental Sciences (IPM), Tehran, Iran49Also at Department of Physics, University of Science and Technology of Mazandaran, Behshahr, Iran.M.GrunewaldUniversity College Dublin, Dublin, IrelandUniversity College DublinDublinIrelandUniversity College Dublin, Dublin, IrelandM.AbbresciaabR.Alyac50A.ColaleoabD.CreanzaacB.D'AnziabN.De FilippisacM.De PalmaabA.Di FlorioacW.Elmetenaweeab50L.FioreaG.IaselliacM.LoukaabG.MaggiacM.MaggiaI.MargjekaabV.MastrapasquaabS.MyabS.NuzzoabA.PellecchiaabA.PompiliabG.PuglieseacR.RadognaaG.Ramirez-SanchezacD.RamosaA.RanieriaL.SilvestrisaF.M.SimoneabÜ.SözbiliraA.StamerraaR.VendittiaP.VerwilligenaA.ZazaabaINFN Sezione di Bari, Bari, ItalyINFN Sezione di BariBariItalyINFN Sezione di Bari, Bari, ItalybUniversità di Bari, Bari, ItalyUniversità di BariBariItalyUniversità di Bari, Bari, ItalycPolitecnico di Bari, Bari, ItalyPolitecnico di BariBariItalyPolitecnico di Bari, Bari, Italy50Also at Helwan University, Cairo, Egypt.G.AbbiendiaC.BattilanaabD.BonacorsiabL.BorgonoviaR.CampaniniabP.CapiluppiabA.CastroabF.R.CavalloaM.CuffianiabG.M.DallavalleaT.DiotaleviabF.FabbriaA.FanfaniabD.FasanellaabP.GiacomelliaL.GiommiabC.GrandiaL.GuiducciabS.Lo Meoa51L.LunertiabS.MarcelliniaG.MasettiaF.L.NavarriaabA.PerrottaaF.PrimaveraabA.M.RossiabG.P.SiroliabaINFN Sezione di Bologna, Bologna, ItalyINFN Sezione di BolognaBolognaItalyINFN Sezione di Bologna, Bologna, ItalybUniversità di Bologna, Bologna, ItalyUniversità di BolognaBolognaItalyUniversità di Bologna, Bologna, Italy51Also at Italian National Agency for New Technologies, Energy and Sustainable Economic Development, Bologna, Italy.S.Costaab52A.Di MattiaaR.PotenzaabA.Tricomiab52C.TuveabaINFN Sezione di Catania, Catania, ItalyINFN Sezione di CataniaCataniaItalyINFN Sezione di Catania, Catania, ItalybUniversità di Catania, Catania, ItalyUniversità di CataniaCataniaItalyUniversità di Catania, Catania, Italy52Also at Centro Siciliano di Fisica Nucleare e di Struttura Della Materia, Catania, Italy.P.AssiourasaG.BarbagliaG.BardelliabB.CamaianiabA.CasseseaR.CeccarelliaV.CiulliabC.CivininiaR.D'AlessandroabE.FocardiabT.KelloaG.LatinoabP.LenziabM.LizzoaM.MeschiniaS.PaolettiaA.PapanastassiouabG.SguazzoniaL.VilianiaaINFN Sezione di Firenze, Firenze, ItalyINFN Sezione di FirenzeFirenzeItalyINFN Sezione di Firenze, Firenze, ItalybUniversità di Firenze, Firenze, ItalyUniversità di FirenzeFirenzeItalyUniversità di Firenze, Firenze, ItalyL.BenussiS.BiancoS.Meola53D.PiccoloINFN Laboratori Nazionali di Frascati, Frascati, ItalyINFN Laboratori Nazionali di FrascatiFrascatiItalyINFN Laboratori Nazionali di Frascati, Frascati, Italy53Also at Università degli Studi Guglielmo Marconi, Roma, Italy.P.ChatagnonaF.FerroaE.RobuttiaS.TosiabaINFN Sezione di Genova, Genova, ItalyINFN Sezione di GenovaGenovaItalyINFN Sezione di Genova, Genova, ItalybUniversità di Genova, Genova, ItalyUniversità di GenovaGenovaItalyUniversità di Genova, Genova, ItalyA.BenagliaaG.BoldriniabF.BrivioaF.CetorelliaF.De GuioabM.E.DinardoabP.DiniaS.GennaiaR.GerosaabA.GhezziabP.GovoniabL.GuzziaM.T.LucchiniabM.MalbertiaS.MalvezziaA.MassironiaD.MenasceaL.MoroniaM.PaganoniabD.PedriniaB.S.PinoliniaS.RagazziabT.Tabarelli de FatisabD.ZuoloaaINFN Sezione di Milano-Bicocca, Milano, ItalyINFN Sezione di Milano-BicoccaMilanoItalyINFN Sezione di Milano-Bicocca, Milano, ItalybUniversità di Milano-Bicocca, Milano, ItalyUniversità di Milano-BicoccaMilanoItalyUniversità di Milano-Bicocca, Milano, ItalyS.BuontempoaA.CagnottaabF.CarnevaliabN.CavalloacA.De IorioabF.FabozziacA.O.M.IorioabL.Listaab54P.Paoluccia33B.RossiaC.SciaccaabaINFN Sezione di Napoli, Napoli, ItalyINFN Sezione di NapoliNapoliItalyINFN Sezione di Napoli, Napoli, ItalybUniversità di Napoli ‘Federico II’, Napoli, ItalyUniversità di Napoli ‘Federico II’NapoliItalyUniversità di Napoli ‘Federico II’, Napoli, ItalycUniversità della Basilicata, Potenza, ItalyUniversità della BasilicataPotenzaItalyUniversità della Basilicata, Potenza, ItalydUniversità G. Marconi, Roma, ItalyUniversità G. MarconiRomaItalyUniversità G. Marconi, Roma, Italy54Also at Scuola Superiore Meridionale, Università di Napoli ‘Federico II’, Napoli, Italy.R.ArdinoaP.AzziaN.Bacchettaa55D.BiselloabP.BortignonaA.BragagnoloabR.CarlinabP.ChecchiaaT.DorigoaF.FanzagoaU.GaspariniabF.GonellaaE.LusianiaM.MargoniabM.MiglioriniabJ.PazziniabP.RoncheseabR.RossinabF.SimonettoabG.StrongaM.TosiabA.TriossiabS.VenturaaH.YararabM.ZanettiabP.ZottoabA.ZucchettaabG.ZumerleabaINFN Sezione di Padova, Padova, ItalyINFN Sezione di PadovaPadovaItalyINFN Sezione di Padova, Padova, ItalybUniversità di Padova, Padova, ItalyUniversità di PadovaPadovaItalyUniversità di Padova, Padova, ItalycUniversità di Trento, Trento, ItalyUniversità di TrentoTrentoItalyUniversità di Trento, Trento, Italy55Also at Fermi National Accelerator Laboratory, Batavia, Illinois, USA.S.Abu Zeida56C.AimèabA.BraghieriaS.CalzaferriaD.FiorinaaP.MontagnaabV.ReaC.RiccardiabP.SalviniaI.VaiabP.VituloabaINFN Sezione di Pavia, Pavia, ItalyINFN Sezione di PaviaPaviaItalyINFN Sezione di Pavia, Pavia, ItalybUniversità di Pavia, Pavia, ItalyUniversità di PaviaPaviaItalyUniversità di Pavia, Pavia, Italy56Also at Ain Shams University, Cairo, Egypt.S.AjmalabP.Asenova57G.M.BileiaD.CiangottiniabL.FanòabM.MagheriniabG.MantovaniabV.MarianiabM.MenichelliaF.Moscatellia57A.RossiabA.SantocchiaabD.SpigaaT.TedeschiabaINFN Sezione di Perugia, Perugia, ItalyINFN Sezione di PerugiaPerugiaItalyINFN Sezione di Perugia, Perugia, ItalybUniversità di Perugia, Perugia, ItalyUniversità di PerugiaPerugiaItalyUniversità di Perugia, Perugia, Italy57Also at Consiglio Nazionale delle Ricerche - Istituto Officina dei Materiali, Perugia, Italy.P.AzzurriaG.BagliesiaR.BhattacharyaaL.BianchiniabT.BoccaliaE.BossiniaD.BruschiniacR.CastaldiaM.A.CiocciabM.CiprianiabV.D'AmanteadR.Dell'OrsoaS.DonatoaA.GiassiaF.LigabueacD.Matos FigueiredoaA.MessineoabM.MusichabF.PallaaA.RizziabG.RolandiacS.Roy ChowdhuryaT.SarkaraA.ScribanoaP.SpagnoloaR.TenchiniaG.TonelliabN.TuriniadA.VenturiaP.G.VerdiniaaINFN Sezione di Pisa, Pisa, ItalyINFN Sezione di PisaPisaItalyINFN Sezione di Pisa, Pisa, ItalybUniversità di Pisa, Pisa, ItalyUniversità di PisaPisaItalyUniversità di Pisa, Pisa, ItalycScuola Normale Superiore di Pisa, Pisa, ItalyScuola Normale Superiore di PisaPisaItalyScuola Normale Superiore di Pisa, Pisa, ItalydUniversità di Siena, Siena, ItalyUniversità di SienaSienaItalyUniversità di Siena, Siena, ItalyP.BarriaaM.CampanaabF.CavallariaL.Cunqueiro MendezabD.Del ReabE.Di MarcoaM.DiemozaF.ErricoabE.LongoabP.MeridianiaJ.MijuskovicabG.OrgantiniabF.PandolfiaR.ParamattiabC.QuarantaabS.RahatlouabC.RovelliaF.SantanastasioabL.SoffiaaINFN Sezione di Roma, Roma, ItalyINFN Sezione di RomaRomaItalyINFN Sezione di Roma, Roma, ItalybSapienza Università di Roma, Roma, ItalySapienza Università di RomaRomaItalySapienza Università di Roma, Roma, ItalyN.AmapaneabR.ArcidiaconoacS.ArgiroabM.ArneodoacN.BartosikaR.BellanabA.BelloraabC.BiinoaN.CartigliaaM.CostaabR.CovarelliabN.DemariaaL.FincoaM.GrippoabB.KianiabF.LeggeraF.LuongoabC.MariottiaS.MaselliaA.MeccaabE.MiglioreabM.MontenoaR.MulargiaaM.M.ObertinoabG.OrtonaaL.PacherabN.PastroneaM.PelliccioniaM.RuspaacF.SivieroabV.SolaabA.SolanoabA.StaianoaC.TarriconeabD.TrocinoaG.UmoretabE.VlasovabaINFN Sezione di Torino, Torino, ItalyINFN Sezione di TorinoTorinoItalyINFN Sezione di Torino, Torino, ItalybUniversità di Torino, Torino, ItalyUniversità di TorinoTorinoItalyUniversità di Torino, Torino, ItalycUniversità del Piemonte Orientale, Novara, ItalyUniversità del Piemonte OrientaleNovaraItalyUniversità del Piemonte Orientale, Novara, ItalyS.BelforteaV.CandeliseabM.CasarsaaF.CossuttiaK.De LeoabG.Della RiccaabaINFN Sezione di Trieste, Trieste, ItalyINFN Sezione di TriesteTriesteItalyINFN Sezione di Trieste, Trieste, ItalybUniversità di Trieste, Trieste, ItalyUniversità di TriesteTriesteItalyUniversità di Trieste, Trieste, ItalyS.DograJ.HongC.HuhB.KimD.H.KimJ.KimH.LeeS.W.LeeC.S.MoonY.D.OhM.S.RyuS.SekmenY.C.YangKyungpook National University, Daegu, KoreaKyungpook National UniversityDaeguKoreaKyungpook National University, Daegu, KoreaM.S.KimDepartment of Mathematics and Physics - GWNU, Gangneung, KoreaDepartment of Mathematics and Physics - GWNUGangneungKoreaDepartment of Mathematics and Physics - GWNU, Gangneung, KoreaG.BakP.GwakH.KimD.H.MoonChonnam National University, Institute for Universe and Elementary Particles, Kwangju, KoreaChonnam National UniversityInstitute for Universe and Elementary ParticlesKwangjuKoreaChonnam National University, Institute for Universe and Elementary Particles, Kwangju, KoreaE.AsilarD.KimT.J.KimJ.A.MerlinHanyang University, Seoul, KoreaHanyang UniversitySeoulKoreaHanyang University, Seoul, KoreaS.ChoiS.HanB.HongK.LeeK.S.LeeS.LeeJ.ParkS.K.ParkJ.YooKorea University, Seoul, KoreaKorea UniversitySeoulKoreaKorea University, Seoul, KoreaJ.GohS.YangKyung Hee University, Department of Physics, Seoul, KoreaKyung Hee UniversityDepartment of PhysicsSeoulKoreaKyung Hee University, Department of Physics, Seoul, KoreaH.S.KimY.KimS.LeeSejong University, Seoul, KoreaSejong UniversitySeoulKoreaSejong University, Seoul, KoreaJ.AlmondJ.H.BhyunJ.ChoiW.JunJ.KimJ.S.KimS.KoH.KwonH.LeeJ.LeeJ.LeeB.H.OhS.B.OhH.SeoU.K.YangI.YoonSeoul National University, Seoul, KoreaSeoul National UniversitySeoulKoreaSeoul National University, Seoul, KoreaW.JangD.Y.KangY.KangS.KimB.KoJ.S.H.LeeY.LeeI.C.ParkY.RohI.J.WatsonUniversity of Seoul, Seoul, KoreaUniversity of SeoulSeoulKoreaUniversity of Seoul, Seoul, KoreaS.HaH.D.YooYonsei University, Department of Physics, Seoul, KoreaYonsei UniversityDepartment of PhysicsSeoulKoreaYonsei University, Department of Physics, Seoul, KoreaM.ChoiM.R.KimH.LeeY.LeeI.YuSungkyunkwan University, Suwon, KoreaSungkyunkwan UniversitySuwonKoreaSungkyunkwan University, Suwon, KoreaT.BeyrouthyY.MaghrbiCollege of Engineering and Technology, American University of the Middle East (AUM), Dasman, KuwaitCollege of Engineering and TechnologyAmerican University of the Middle East (AUM)DasmanKuwaitCollege of Engineering and Technology, American University of the Middle East (AUM), Dasman, KuwaitK.DreimanisA.GaileG.PikursA.PotrebkoM.SeidelV.Veckalns58Riga Technical University, Riga, LatviaRiga Technical UniversityRigaLatviaRiga Technical University, Riga, Latvia58Also at Riga Technical University, Riga, Latvia.N.R.StrautnieksUniversity of Latvia (LU), Riga, LatviaUniversity of Latvia (LU)RigaLatviaUniversity of Latvia (LU), Riga, LatviaM.AmbrozasA.JuodagalvisA.RinkeviciusG.TamulaitisVilnius University, Vilnius, LithuaniaVilnius UniversityVilniusLithuaniaVilnius University, Vilnius, LithuaniaN.Bin NorjoharuddeenI.Yusuff59Z.ZolkapliNational Centre for Particle Physics, Universiti Malaya, Kuala Lumpur, MalaysiaNational Centre for Particle PhysicsUniversiti MalayaKuala LumpurMalaysiaNational Centre for Particle Physics, Universiti Malaya, Kuala Lumpur, Malaysia59Also at Department of Applied Physics, Faculty of Science and Technology, Universiti Kebangsaan Malaysia, Bangi, Malaysia.J.F.BenitezA.Castaneda HernandezH.A.Encinas AcostaL.G.Gallegos MaríñezM.León CoelloJ.A.Murillo QuijadaA.SehrawatL.Valencia PalomoUniversidad de Sonora (UNISON), Hermosillo, MexicoUniversidad de Sonora (UNISON)HermosilloMexicoUniversidad de Sonora (UNISON), Hermosillo, MexicoG.AyalaH.Castilla-ValdezE.De La Cruz-BureloI.Heredia-De La Cruz60R.Lopez-FernandezC.A.Mondragon HerreraA.Sánchez HernándezCentro de Investigacion y de Estudios Avanzados del IPN, Mexico City, MexicoCentro de Investigacion y de Estudios Avanzados del IPNMexico CityMexicoCentro de Investigacion y de Estudios Avanzados del IPN, Mexico City, Mexico60Also at Consejo Nacional de Ciencia y Tecnología, Mexico City, Mexico.C.Oropeza BarreraM.Ramírez GarcíaUniversidad Iberoamericana, Mexico City, MexicoUniversidad IberoamericanaMexico CityMexicoUniversidad Iberoamericana, Mexico City, MexicoI.BautistaI.PedrazaH.A.Salazar IbarguenC.Uribe EstradaBenemerita Universidad Autonoma de Puebla, Puebla, MexicoBenemerita Universidad Autonoma de PueblaPueblaMexicoBenemerita Universidad Autonoma de Puebla, Puebla, MexicoI.BubanjaN.RaicevicUniversity of Montenegro, Podgorica, MontenegroUniversity of MontenegroPodgoricaMontenegroUniversity of Montenegro, Podgorica, MontenegroP.H.ButlerUniversity of Canterbury, Christchurch, New ZealandUniversity of CanterburyChristchurchNew ZealandUniversity of Canterbury, Christchurch, New ZealandA.AhmadM.I.AsgharA.AwaisM.I.M.AwanH.R.HooraniW.A.KhanNational Centre for Physics, Quaid-I-Azam University, Islamabad, PakistanNational Centre for PhysicsQuaid-I-Azam UniversityIslamabadPakistanNational Centre for Physics, Quaid-I-Azam University, Islamabad, PakistanV.AvatiL.GrzankaM.MalawskiAGH University of Krakow, Faculty of Computer Science, Electronics and Telecommunications, Krakow, PolandAGH University of KrakowFaculty of Computer Science, Electronics and TelecommunicationsKrakowPolandAGH University of Krakow, Faculty of Computer Science, Electronics and Telecommunications, Krakow, PolandH.BialkowskaM.BlujB.BoimskaM.GórskiM.KazanaM.SzleperP.ZalewskiNational Centre for Nuclear Research, Swierk, PolandNational Centre for Nuclear ResearchSwierkPolandNational Centre for Nuclear Research, Swierk, PolandK.BunkowskiK.DorobaA.KalinowskiM.KoneckiJ.KrolikowskiA.MuhammadInstitute of Experimental Physics, Faculty of Physics, University of Warsaw, Warsaw, PolandInstitute of Experimental PhysicsFaculty of PhysicsUniversity of WarsawWarsawPolandInstitute of Experimental Physics, Faculty of Physics, University of Warsaw, Warsaw, PolandK.PozniakW.ZabolotnyWarsaw University of Technology, Warsaw, PolandWarsaw University of TechnologyWarsawPolandWarsaw University of Technology, Warsaw, PolandM.AraujoD.BastosC.Beirão Da Cruz E SilvaA.BolettiM.BozzoT.CamporesiG.Da MolinP.FaccioliM.GallinaroJ.HollarN.LeonardoT.NiknejadA.PetrilliM.PisanoJ.SeixasJ.VarelaJ.W.WulffLaboratório de Instrumentação e Física Experimental de Partículas, Lisboa, PortugalLaboratório de Instrumentação e Física Experimental de PartículasLisboaPortugalLaboratório de Instrumentação e Física Experimental de Partículas, Lisboa, PortugalP.AdzicP.MilenovicFaculty of Physics, University of Belgrade, Belgrade, SerbiaFaculty of PhysicsUniversity of BelgradeBelgradeSerbiaFaculty of Physics, University of Belgrade, Belgrade, SerbiaM.DordevicJ.MilosevicV.RekovicVINCA Institute of Nuclear Sciences, University of Belgrade, Belgrade, SerbiaVINCA Institute of Nuclear SciencesUniversity of BelgradeBelgradeSerbiaVINCA Institute of Nuclear Sciences, University of Belgrade, Belgrade, SerbiaM.Aguilar-BenitezJ.Alcaraz MaestreCristina F.BedoyaM.CepedaM.CerradaN.ColinoB.De La CruzA.Delgado PerisA.Escalante Del ValleD.Fernández Del ValJ.P.Fernández RamosJ.FlixM.C.FouzO.Gonzalez LopezS.Goy LopezJ.M.HernandezM.I.JosaD.MoranC.M.Morcillo PerezÁ.Navarro TobarC.Perez DengraA.Pérez-Calero YzquierdoJ.Puerta PelayoI.RedondoD.D.Redondo FerreroL.RomeroS.Sánchez NavasL.Urda GómezJ.Vazquez EscobarC.WillmottCentro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, SpainCentro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT)MadridSpainCentro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, SpainJ.F.de TrocónizUniversidad Autónoma de Madrid, Madrid, SpainUniversidad Autónoma de MadridMadridSpainUniversidad Autónoma de Madrid, Madrid, SpainB.Alvarez GonzalezJ.CuevasJ.Fernandez MenendezS.FolguerasI.Gonzalez CaballeroJ.R.González FernándezE.Palencia CortezonC.Ramón ÁlvarezV.Rodríguez BouzaA.Soto RodríguezA.TrapoteC.Vico VillalbaP.VischiaUniversidad de Oviedo, Instituto Universitario de Ciencias y Tecnologías Espaciales de Asturias (ICTEA), Oviedo, SpainUniversidad de OviedoInstituto Universitario de Ciencias y Tecnologías Espaciales de Asturias (ICTEA)OviedoSpainUniversidad de Oviedo, Instituto Universitario de Ciencias y Tecnologías Espaciales de Asturias (ICTEA), Oviedo, SpainS.BhowmikS.Blanco FernándezJ.A.Brochero CifuentesI.J.CabrilloA.CalderonJ.Duarte CampderrosM.FernandezG.GomezC.Lasaosa GarcíaC.Martinez RiveroP.Martinez Ruiz del ArbolF.MatorrasP.Matorras CuevasE.Navarrete RamosJ.Piedra GomezL.ScodellaroI.VilaJ.M.Vizan GarciaInstituto de Física de Cantabria (IFCA), CSIC-Universidad de Cantabria, Santander, SpainInstituto de Física de Cantabria (IFCA)CSIC-Universidad de CantabriaSantanderSpainInstituto de Física de Cantabria (IFCA), CSIC-Universidad de Cantabria, Santander, SpainM.K.JayanandaB.Kailasapathy61D.U.J.SonnadaraD.D.C.WickramarathnaUniversity of Colombo, Colombo, Sri LankaUniversity of ColomboColomboSri LankaUniversity of Colombo, Colombo, Sri Lanka61Also at Trincomalee Campus, Eastern University, Sri Lanka, Nilaveli, Sri Lanka.W.G.D.Dharmaratna62K.LiyanageN.PereraN.WickramageUniversity of Ruhuna, Department of Physics, Matara, Sri LankaUniversity of RuhunaDepartment of PhysicsMataraSri LankaUniversity of Ruhuna, Department of Physics, Matara, Sri Lanka62Also at Saegis Campus, Nugegoda, Sri Lanka.D.AbbaneoC.AmendolaE.AuffrayG.AuzingerJ.BaechlerD.BarneyA.Bermúdez MartínezM.BiancoB.BilinA.A.Bin AnuarA.BocciE.BrondolinC.CaillolG.CerminaraN.ChernyavskayaD.d'EnterriaA.DabrowskiA.DavidA.De RoeckM.M.DefranchisM.DeileM.DobsonF.Fallavollita63L.ForthommeG.FranzoniW.FunkS.GianiD.GigiK.GillF.GlegeL.GouskosM.HarankoJ.HegemanB.HuberV.InnocenteT.JamesP.JanotS.LaurilaP.LecoqE.LeutgebC.LourençoB.MaierL.MalgeriM.MannelliA.C.MariniM.MatthewmanF.MeijersS.MersiE.MeschiV.MilosevicF.MontiF.MoortgatM.MuldersI.NeutelingsS.OrfanelliF.PantaleoG.PetruccianiA.PfeifferM.PieriniD.PiparoH.QuD.RabadyG.Reales GutiérrezM.RovereH.SakulinS.ScarfiC.SchwickM.SelvaggiA.SharmaK.ShchelinaP.SilvaP.Sphicas64A.G.Stahl LeitonA.SteenS.SummersD.TreilleP.TropeaA.TsirouD.WalterJ.Wanczyk65J.WangS.WuchterlP.ZehetnerP.ZejdlW.D.ZeunerCERN, European Organization for Nuclear Research, Geneva, SwitzerlandCERNEuropean Organization for Nuclear ResearchGenevaSwitzerlandCERN, European Organization for Nuclear Research, Geneva, Switzerland63Also at INFN Sezione di Pavia, Università di Pavia, Pavia, Italy.64Also at National and Kapodistrian University of Athens, Athens, Greece.65Also at Ecole Polytechnique Fédérale Lausanne, Lausanne, Switzerland.T.Bevilacqua66L.Caminada66A.EbrahimiW.ErdmannR.HorisbergerQ.IngramH.C.KaestliD.KotlinskiC.LangeM.Missiroli66L.Noehte66T.RohePaul Scherrer Institut, Villigen, SwitzerlandPaul Scherrer InstitutVilligenSwitzerlandPaul Scherrer Institut, Villigen, Switzerland66Also at Universität Zürich, Zurich, Switzerland.T.K.AarrestadK.Androsov65M.BackhausA.CalandriC.CazzanigaK.DattaA.De CosaG.DissertoriM.DittmarM.DonegàF.EbleM.GalliK.GediaF.GlessgenC.GrabD.HitsW.LustermannA.-M.LyonR.A.ManzoniM.MarchegianiL.MarcheseC.Martin PerezA.Mascellani65F.Nessi-TedaldiF.PaussV.PerovicS.PigazziniM.ReichmannC.ReisselT.ReitenspiessB.RisticF.RitiD.RuiniD.A.Sanz BecerraR.SeiditaJ.Steggemann65D.ValsecchiR.WallnyETH Zurich - Institute for Particle Physics and Astrophysics (IPA), Zurich, SwitzerlandETH ZurichInstitute for Particle Physics and Astrophysics (IPA)ZurichSwitzerlandETH Zurich - Institute for Particle Physics and Astrophysics (IPA), Zurich, SwitzerlandC.Amsler67P.BärtschiC.BottaD.BrzhechkoM.F.CanelliK.CormierR.Del BurgoJ.K.HeikkiläM.HuwilerW.JinA.JofreheiB.KilminsterS.LeontsinisS.P.LiechtiA.MacchioloP.MeiringV.M.MikuniU.MolinattiA.ReimersP.RobmannS.Sanchez CruzK.SchweigerM.SengerY.TakahashiR.TramontanoUniversität Zürich, Zurich, SwitzerlandUniversität ZürichZurichSwitzerlandUniversität Zürich, Zurich, Switzerland67Also at Stefan Meyer Institute for Subatomic Physics, Vienna, Austria.C.Adloff68D.BhowmikC.M.KuoW.LinP.K.RoutP.C.Tiwari42S.S.YuNational Central University, Chung-Li, TaiwanNational Central UniversityChung-LiTaiwanNational Central University, Chung-Li, Taiwan68Also at Laboratoire d'Annecy-le-Vieux de Physique des Particules, IN2P3-CNRS, Annecy-le-Vieux, France.L.CeardY.ChaoK.F.ChenP.s.ChenZ.g.ChenW.-S.HouT.h.HsuY.w.KaoR.KhuranaG.KoleY.y.LiR.-S.LuE.PaganisX.f.SuJ.Thomas-WilskerL.s.TsaiH.y.WuE.YazganNational Taiwan University (NTU), Taipei, TaiwanNational Taiwan University (NTU)TaipeiTaiwanNational Taiwan University (NTU), Taipei, TaiwanC.AsawatangtrakuldeeN.SrimanobhasV.WachirapusitanandHigh Energy Physics Research Unit, Department of Physics, Faculty of Science, Chulalongkorn University, Bangkok, ThailandHigh Energy Physics Research UnitDepartment of PhysicsFaculty of ScienceChulalongkorn UniversityBangkokThailandHigh Energy Physics Research Unit, Department of Physics, Faculty of Science, Chulalongkorn University, Bangkok, ThailandD.AgyelF.BoranZ.S.DemirogluF.DolekI.Dumanoglu69E.EskutY.Guler70E.Gurpinar Guler70C.IsikO.KaraA.Kayis TopaksuU.KiminsuG.OnengutK.Ozdemir71A.PolatozB.Tali72U.G.TokS.TurkcaparE.UslanI.S.ZorbakirÇukurova University, Physics Department, Science and Art Faculty, Adana, TurkeyÇukurova UniversityPhysics DepartmentScience and Art FacultyAdanaTurkeyÇukurova University, Physics Department, Science and Art Faculty, Adana, Turkey69Also at Near East University, Research Center of Experimental Health Science, Mersin, Turkey.70Also at Konya Technical University, Konya, Turkey.71Also at Izmir Bakircay University, Izmir, Turkey.72Also at Adiyaman University, Adiyaman, Turkey.M.Yalvac73Middle East Technical University, Physics Department, Ankara, TurkeyMiddle East Technical UniversityPhysics DepartmentAnkaraTurkeyMiddle East Technical University, Physics Department, Ankara, Turkey73Also at Bozok Universitetesi Rektörlügü, Yozgat, Turkey.B.AkgunI.O.AtakisiE.GülmezM.Kaya74O.Kaya75S.Tekten76Bogazici University, Istanbul, TurkeyBogazici UniversityIstanbulTurkeyBogazici University, Istanbul, Turkey74Also at Marmara University, Istanbul, Turkey.75Also at Milli Savunma University, Istanbul, Turkey.76Also at Kafkas University, Kars, Turkey.A.CakirK.Cankocak6977Y.KomurcuS.Sen78Istanbul Technical University, Istanbul, TurkeyIstanbul Technical UniversityIstanbulTurkeyIstanbul Technical University, Istanbul, Turkey77Now at stanbul Okan University, Istanbul, Turkey.78Also at Hacettepe University, Ankara, Turkey.O.AydilekS.Cerci72V.EpshteynB.HacisahinogluI.Hos79B.KaynakS.OzkorucukluO.PotokH.SertC.SimsekD.Sunar Cerci72C.ZorbilmezIstanbul University, Istanbul, TurkeyIstanbul UniversityIstanbulTurkeyIstanbul University, Istanbul, Turkey79Also at Istanbul University - Cerrahpasa, Faculty of Engineering, Istanbul, Turkey.B.Isildak80Yildiz Technical University, Istanbul, TurkeyYildiz Technical UniversityIstanbulTurkeyYildiz Technical University, Istanbul, Turkey80Also at Yildiz Technical University, Istanbul, Turkey.A.BoyaryntsevB.GrynyovInstitute for Scintillation Materials of National Academy of Science of Ukraine, Kharkiv, UkraineInstitute for Scintillation Materials of National Academy of Science of UkraineKharkivUkraineInstitute for Scintillation Materials of National Academy of Science of Ukraine, Kharkiv, UkraineL.LevchukNational Science Centre, Kharkiv Institute of Physics and Technology, Kharkiv, UkraineNational Science CentreKharkiv Institute of Physics and TechnologyKharkivUkraineNational Science Centre, Kharkiv Institute of Physics and Technology, Kharkiv, UkraineD.AnthonyJ.J.BrookeA.BundockF.BuryE.ClementD.CussansH.FlacherM.GlowackiJ.GoldsteinH.F.HeathL.KreczkoS.ParamesvaranS.Seif El Nasr-StoreyV.J.SmithN.Stylianou81K.Walkingshaw PassR.WhiteUniversity of Bristol, Bristol, United KingdomUniversity of BristolBristolUnited KingdomUniversity of Bristol, Bristol, United Kingdom81Also at Vrije Universiteit Brussel, Brussel, Belgium.A.H.BallK.W.BellA.Belyaev82C.BrewR.M.BrownD.J.A.CockerillC.CookeK.V.EllisK.HarderS.HarperM.-L.Holmberg83J.LinacreK.ManolopoulosD.M.NewboldE.OlaiyaD.PetytT.ReisG.SalviT.SchuhC.H.Shepherd-ThemistocleousI.R.TomalinT.WilliamsRutherford Appleton Laboratory, Didcot, United KingdomRutherford Appleton LaboratoryDidcotUnited KingdomRutherford Appleton Laboratory, Didcot, United Kingdom82Also at School of Physics and Astronomy, University of Southampton, Southampton, United Kingdom.83Also at University of Bristol, Bristol, United Kingdom.R.BainbridgeP.BlochC.E.BrownO.BuchmullerV.CacchioC.A.Carrillo MontoyaG.S.Chahal84D.CollingJ.S.DancuI.DasP.DaunceyG.DaviesJ.DaviesM.Della NegraS.FayerG.FediG.HallM.H.HassanshahiA.HowardG.IlesM.KnightJ.LangfordJ.León HolgadoL.LyonsA.-M.MagnanS.MalikA.MartelliM.MieskolainenJ.Nash85M.PesaresiB.C.Radburn-SmithA.RichardsA.RoseC.SeezR.ShuklaA.TapperK.UchidaG.P.UttleyL.H.VageT.Virdee33M.VojinovicN.WardleD.WinterbottomImperial College, London, United KingdomImperial CollegeLondonUnited KingdomImperial College, London, United Kingdom84Also at IPPP Durham University, Durham, United Kingdom.85Also at Monash University, Faculty of Science, Clayton, Australia.K.ColdhamJ.E.ColeA.KhanP.KyberdI.D.ReidBrunel University, Uxbridge, United KingdomBrunel UniversityUxbridgeUnited KingdomBrunel University, Uxbridge, United KingdomS.AbdullinA.BrinkerhoffB.CarawayJ.DittmannK.HatakeyamaJ.HiltbrandB.McMasterM.SaundersS.SawantC.SutantawibulJ.WilsonBaylor University, Waco, TX, USABaylor UniversityWacoTXUSABaylor University, Waco, Texas, USAR.BartekA.DominguezC.Huerta EscamillaA.E.SimsekR.UniyalA.M.Vargas HernandezCatholic University of America, Washington, DC, USACatholic University of AmericaWashingtonDCUSACatholic University of America, Washington, DC, USAB.BamR.ChudasamaS.I.CooperS.V.GleyzerC.U.PerezP.Rumerio86E.UsaiR.YiThe University of Alabama, Tuscaloosa, AL, USAThe University of AlabamaTuscaloosaALUSAThe University of Alabama, Tuscaloosa, Alabama, USA86Also at Università di Torino, Torino, Italy.A.AkpinarA.AlbertD.ArcaroC.CosbyZ.DemiragliC.EriceC.FangmeierC.Fernandez MadrazoE.FontanesiD.GastlerF.GolfS.JeonI.ReedJ.RohlfK.SalyerD.SperkaD.SpitzbartI.SuarezA.TsatsosS.YuanA.G.ZecchinelliBoston University, Boston, MA, USABoston UniversityBostonMAUSABoston University, Boston, Massachusetts, USAG.BenelliX.Coubez28D.CuttsM.HadleyU.HeintzJ.M.Hogan87T.KwonG.LandsbergK.T.LauD.LiJ.LuoS.MondalM.Narain†N.PervanS.Sagir88F.SimpsonM.StamenkovicW.Y.WongX.YanW.ZhangBrown University, Providence, RI, USABrown UniversityProvidenceRIUSABrown University, Providence, Rhode Island, USA87Also at Bethel University, St. Paul, Minnesota, USA.88Also at Karamanoğlu Mehmetbey University, Karaman, Turkey.S.AbbottJ.BonillaC.BrainerdR.BreedonM.Calderon De La Barca SanchezM.ChertokM.CitronJ.ConwayP.T.CoxR.ErbacherF.JensenO.KukralG.MocellinM.MulhearnD.PellettW.WeiY.YaoF.ZhangUniversity of California, Davis, Davis, CA, USAUniversity of California, DavisDavisCAUSAUniversity of California, Davis, Davis, California, USAM.BachtisR.CousinsA.DattaG.Flores AvilaJ.HauserM.IgnatenkoM.A.IqbalT.LamE.MancaA.Nunez Del PradoD.SaltzbergV.ValuevUniversity of California, Los Angeles, CA, USAUniversity of CaliforniaLos AngelesCAUSAUniversity of California, Los Angeles, California, USAR.ClareJ.W.GaryM.GordonG.HansonW.SiS.Wimpenny†University of California, Riverside, Riverside, CA, USAUniversity of California, RiversideRiversideCAUSAUniversity of California, Riverside, Riverside, California, USAJ.G.BransonS.CittolinS.CoopersteinD.DiazJ.DuarteL.GianniniJ.GuiangR.KansalV.KrutelyovR.LeeJ.LettsM.MasciovecchioF.MokhtarS.MukherjeeM.PieriM.QuinnanB.V.Sathia NarayananV.SharmaM.TadelE.VourliotisF.WürthweinY.XiangA.YagilUniversity of California, San Diego, La Jolla, CA, USAUniversity of California, San DiegoLa JollaCAUSAUniversity of California, San Diego, La Jolla, California, USAA.BarzdukasL.BrennanC.CampagnariA.DorsettJ.IncandelaJ.KimA.J.LiP.MastersonH.MeiJ.RichmanU.SaricaR.SchmitzF.SettiJ.SheplockD.StuartT.Á.VámiS.WangUniversity of California, Santa Barbara - Department of Physics, Santa Barbara, CA, USAUniversity of California, Santa BarbaraDepartment of PhysicsSanta BarbaraCAUSAUniversity of California, Santa Barbara - Department of Physics, Santa Barbara, California, USAA.BornheimO.CerriA.LatorreJ.MaoH.B.NewmanM.SpiropuluJ.R.VlimantC.WangS.XieR.Y.ZhuCalifornia Institute of Technology, Pasadena, CA, USACalifornia Institute of TechnologyPasadenaCAUSACalifornia Institute of Technology, Pasadena, California, USAJ.AlisonS.AnM.B.AndrewsP.BryantM.CremonesiV.DuttaT.FergusonA.HarilalC.LiuT.MudholkarS.MurthyM.PauliniA.RobertsA.SanchezW.TerrillCarnegie Mellon University, Pittsburgh, PA, USACarnegie Mellon UniversityPittsburghPAUSACarnegie Mellon University, Pittsburgh, Pennsylvania, USAJ.P.CumalatW.T.FordA.HassaniG.KarathanasisE.MacDonaldN.ManganelliF.MariniA.PerloffC.SavardN.SchonbeckK.StensonK.A.UlmerS.R.WagnerN.ZipperUniversity of Colorado Boulder, Boulder, CO, USAUniversity of Colorado BoulderBoulderCOUSAUniversity of Colorado Boulder, Boulder, Colorado, USAJ.AlexanderS.Bright-ThonneyX.ChenD.J.CranshawJ.FanX.FanD.GadkariS.HoganP.KotamnivesJ.MonroyM.OshiroJ.R.PattersonJ.ReichertM.ReidA.RydJ.ThomP.WittichR.ZouCornell University, Ithaca, NY, USACornell UniversityIthacaNYUSACornell University, Ithaca, New York, USAM.AlbrowM.AlyariO.AmramG.ApollinariA.ApresyanL.A.T.BauerdickD.BerryJ.BerryhillP.C.BhatK.BurkettJ.N.ButlerA.CanepaG.B.CeratiH.W.K.CheungF.ChlebanaG.CummingsJ.DickinsonI.DuttaV.D.ElviraY.FengJ.FreemanA.GandrakotaZ.GecseL.GrayD.GreenA.GrummerS.GrünendahlD.GuerreroO.GutscheR.M.HarrisR.HellerT.C.HerwigJ.HirschauerL.HorynB.JayatilakaS.JindarianiM.JohnsonU.JoshiT.KlijnsmaB.KlimaK.H.M.KwokS.LammelD.LincolnR.LiptonT.LiuC.MadridK.MaeshimaC.MantillaD.MasonP.McBrideP.MerkelS.MrennaS.NahnJ.NgadiubaD.NoonanV.PapadimitriouN.PastikaK.PedroC.Pena89F.RaveraA.Reinsvold Hall90L.RistoriE.Sexton-KennedyN.SmithA.SohaL.SpiegelS.StoynevJ.StraitL.TaylorS.TkaczykN.V.TranL.UpleggerE.W.VaanderingI.ZoiFermi National Accelerator Laboratory, Batavia, IL, USAFermi National Accelerator LaboratoryBataviaILUSAFermi National Accelerator Laboratory, Batavia, Illinois, USA89Also at California Institute of Technology, Pasadena, California, USA.90Also at United States Naval Academy, Annapolis, Maryland, USA.C.ArutaP.AveryD.BourilkovL.CadamuroP.ChangV.CherepanovR.D.FieldE.KoenigM.KolosovaJ.KonigsbergA.KorytovK.H.LoK.MatchevN.MenendezG.MitselmakherK.MohrmanA.Muthirakalayil MadhuN.RawalD.RosenzweigS.RosenzweigK.ShiJ.WangUniversity of Florida, Gainesville, FL, USAUniversity of FloridaGainesvilleFLUSAUniversity of Florida, Gainesville, Florida, USAT.AdamsA.Al KadhimA.AskewN.BowerR.HabibullahV.HagopianR.HashmiR.S.KimS.KimT.KolbergG.MartinezH.ProsperP.R.ProvaO.ViazloM.WulansatitiR.YohayJ.ZhangFlorida State University, Tallahassee, FL, USAFlorida State UniversityTallahasseeFLUSAFlorida State University, Tallahassee, Florida, USAB.AlsufyaniM.M.BaarmandS.ButallaT.Elkafrawy56M.HohlmannR.Kumar VermaM.RahmaniE.YanesFlorida Institute of Technology, Melbourne, FL, USAFlorida Institute of TechnologyMelbourneFLUSAFlorida Institute of Technology, Melbourne, Florida, USAM.R.AdamsA.BatyC.BennettR.CavanaughS.DittmerR.Escobar FrancoO.EvdokimovC.E.GerberD.J.HofmanJ.h.LeeD.S.LemosA.H.MerritC.MillsS.NandaG.OhB.OzekD.PilipovicR.PradhanT.RoyS.RudrabhatlaM.B.TonjesN.VarelasX.WangZ.YeJ.YooUniversity of Illinois Chicago, Chicago, USAUniversity of Illinois ChicagoChicagoUSAUniversity of Illinois Chicago, Chicago, USA, Chicago, USAM.AlhusseiniD.BlendK.Dilsiz91L.EmediatoG.KaramanO.K.KöseyanJ.-P.MerloA.Mestvirishvili92J.NachtmanO.NeogiH.Ogul93Y.OnelA.PenzoC.SnyderE.Tiras94The University of Iowa, Iowa City, IA, USAThe University of IowaIowa CityIAUSAThe University of Iowa, Iowa City, Iowa, USA91Also at Bingol University, Bingol, Turkey.92Also at Georgian Technical University, Tbilisi, Georgia.93Also at Sinop University, Sinop, Turkey.94Also at Erciyes University, Kayseri, Turkey.B.BlumenfeldL.CorcodilosJ.DavisA.V.GritsanL.KangS.KyriacouP.MaksimovicM.RoguljicJ.RoskesS.SekharM.SwartzJohns Hopkins University, Baltimore, MD, USAJohns Hopkins UniversityBaltimoreMDUSAJohns Hopkins University, Baltimore, Maryland, USAA.AbreuL.F.Alcerro AlcerroJ.AnguianoP.BaringerA.BeanZ.FlowersD.GroveJ.KingG.KrintirasM.LazarovitsC.Le MahieuC.LindseyJ.MarquezN.MinafraM.MurrayM.NickelM.PittS.Popescu95C.RoganC.RoyonR.SalvaticoS.SandersC.SmithQ.WangG.WilsonThe University of Kansas, Lawrence, KS, USAThe University of KansasLawrenceKSUSAThe University of Kansas, Lawrence, Kansas, USA95Also at Horia Hulubei National Institute of Physics and Nuclear Engineering (IFIN-HH), Bucharest, Romania.B.AllmondA.IvanovK.KaadzeA.KalogeropoulosD.KimY.MaravinK.NamJ.NatoliD.RoyG.SorrentinoKansas State University, Manhattan, KS, USAKansas State UniversityManhattanKSUSAKansas State University, Manhattan, Kansas, USAF.RebassooD.WrightLawrence Livermore National Laboratory, Livermore, CA, USALawrence Livermore National LaboratoryLivermoreCAUSALawrence Livermore National Laboratory, Livermore, California, 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Mississippi, Oxford, MS, USAUniversity of MississippiOxfordMSUSAUniversity of Mississippi, Oxford, Mississippi, USAK.BloomM.BrysonD.R.ClaesG.HazaJ.HossainC.JooI.KravchenkoJ.E.SiadoW.TabbA.VagneriniA.WightmanF.YanD.YuUniversity of Nebraska-Lincoln, Lincoln, NE, USAUniversity of Nebraska-LincolnLincolnNEUSAUniversity of Nebraska-Lincoln, Lincoln, Nebraska, USAH.BandyopadhyayL.HayI.IashviliA.KharchilavaM.MorrisD.NguyenS.RappoccioH.Rejeb SfarA.WilliamsState University of New York at Buffalo, Buffalo, NY, USAState University of New York at BuffaloBuffaloNYUSAState University of New York at Buffalo, Buffalo, New York, USAG.AlversonE.BarberisJ.DervanY.HaddadY.HanA.KrishnaJ.LiM.Lu96G.MadiganR.MccarthyD.M.MorseV.NguyenT.OrimotoA.ParkerL.SkinnariA.Tishelman-CharnyB.WangD.WoodNortheastern University, Boston, MA, USANortheastern UniversityBostonMAUSANortheastern University, Boston, Massachusetts, USA96Also at Sun Yat-Sen University, Guangzhou, China.S.BhattacharyaJ.BueghlyZ.ChenK.A.HahnY.LiuY.MiaoD.G.MonkM.H.SchmittA.TaliercioM.VelascoNorthwestern University, Evanston, IL, USANorthwestern UniversityEvanstonILUSANorthwestern University, Evanston, Illinois, USAG.AgarwalR.BandR.BucciS.CastellsA.DasR.GoldouzianM.HildrethK.W.HoK.Hurtado AnampaT.IvanovC.JessopK.LannonJ.LawrenceN.LoukasL.LuttonJ.MarianoN.MarinelliI.McalisterT.McCauleyC.McgradyC.MooreY.Musienko17H.NelsonM.OshersonA.PiccinelliR.RuchtiA.TownsendY.WanM.WayneH.YockeyM.ZaruckiL.ZygalaUniversity of Notre Dame, Notre Dame, IN, USAUniversity of Notre DameNotre DameINUSAUniversity of Notre Dame, Notre Dame, Indiana, USAA.BasnetB.BylsmaM.CarriganL.S.DurkinC.HillM.JoyceM.Nunez OrnelasK.WeiB.L.WinerB.R.YatesThe Ohio State University, Columbus, OH, USAThe Ohio State UniversityColumbusOHUSAThe Ohio State University, Columbus, Ohio, 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ColinB.P.PadleyR.RedjimiJ.RotterE.YigitbasiY.ZhangRice University, Houston, TX, USARice UniversityHoustonTXUSARice University, Houston, Texas, USAA.BodekP.de BarbaroR.DeminaJ.L.DulembaC.FallonA.Garcia-BellidoO.HindrichsA.KhukhunaishviliN.ParmarP.Parygin34E.Popova34R.TausG.P.Van OnsemUniversity of Rochester, Rochester, NY, USAUniversity of RochesterRochesterNYUSAUniversity of Rochester, Rochester, New York, USAK.GoulianosThe Rockefeller University, New York, NY, USAThe Rockefeller UniversityNew YorkNYUSAThe Rockefeller University, New York, New York, USAB.ChiaritoJ.P.ChouY.GershteinE.HalkiadakisA.HartM.HeindlD.JaroslawskiO.Karacheban31I.LaflotteA.LathR.MontalvoK.NashH.RoutrayS.SalurS.SchnetzerS.SomalwarR.StoneS.A.ThayilS.ThomasJ.VoraH.WangRutgers, The State University of New Jersey, Piscataway, NJ, USARutgers, The State University of New JerseyPiscatawayNJUSARutgers, The State University of New Jersey, Piscataway, New Jersey, USAH.AcharyaD.AllyA.G.DelannoyS.FiorendiS.HigginbothamT.HolmesA.R.KanugantiN.KarunarathnaL.LeeE.NibigiraS.SpanierUniversity of Tennessee, Knoxville, TN, USAUniversity of TennesseeKnoxvilleTNUSAUniversity of Tennessee, Knoxville, Tennessee, USAD.AebiM.AhmadO.Bouhali97M.DalchenkoR.EusebiJ.GilmoreT.HuangT.Kamon98H.KimS.LuoS.MalhotraR.MuellerD.OvertonD.RathjensA.SafonovTexas A&M University, College Station, TX, USATexas A&M UniversityCollege StationTXUSATexas A&M University, College Station, Texas, USA97Also at Texas A&M University at Qatar, Doha, Qatar.98Also at Kyungpook National University, Daegu, Korea.N.AkchurinJ.DamgovV.HegdeA.HussainY.KazhykarimK.LamichhaneS.W.LeeA.MankelT.PeltolaI.VolobouevA.WhitbeckTexas Tech University, Lubbock, TX, USATexas Tech UniversityLubbockTXUSATexas Tech University, Lubbock, Texas, USAE.AppeltS.GreeneA.GurrolaW.JohnsR.Kunnawalkam ElayavalliA.MeloF.RomeoP.SheldonS.TuoJ.VelkovskaJ.ViinikainenVanderbilt University, Nashville, TN, USAVanderbilt UniversityNashvilleTNUSAVanderbilt University, Nashville, Tennessee, USAB.CardwellB.CoxJ.HakalaR.HiroskyA.LedovskoyC.NeuC.E.Perez LaraUniversity of Virginia, Charlottesville, VA, USAUniversity of VirginiaCharlottesvilleVAUSAUniversity of Virginia, Charlottesville, Virginia, USAP.E.KarchinWayne State University, Detroit, MI, USAWayne State UniversityDetroitMIUSAWayne State University, Detroit, Michigan, USAA.AravindS.BanerjeeK.BlackT.BoseS.DasuI.De BruynP.EveraertsC.GalloniH.HeM.HerndonA.HerveC.K.KorakaA.LanaroR.LovelessJ.Madhusudanan SreekalaA.MallampalliA.MohammadiS.MondalG.ParidaD.PinnaA.SavinV.ShangV.SharmaW.H.SmithD.TeagueH.F.TsoiW.VetensA.WardenUniversity of Wisconsin - Madison, Madison, WI, USAUniversity of Wisconsin - MadisonMadisonWIUSAUniversity of Wisconsin - Madison, Madison, Wisconsin, USAS.AfanasievV.AndreevYu.AndreevT.AushevM.AzarkinA.BabaevA.BelyaevV.Blinov99E.BoosV.BorshchD.BudkouskiV.BunichevV.ChekhovskyR.Chistov99M.Danilov99A.DermenevT.Dimova99D.Druzhkin100M.Dubinin89L.DudkoA.ErshovG.GavrilovV.GavrilovS.GninenkoV.GolovtcovN.GolubevI.GolutvinI.GorbunovA.GribushinY.IvanovV.KachanovV.KarjavineA.KarneyeuV.Kim99M.KirakosyanD.KirpichnikovM.KirsanovV.KlyukhinV.KorenkovA.Kozyrev99N.KrasnikovA.LanevP.Levchenko101N.LychkovskayaV.MakarenkoA.MalakhovV.Matveev99V.MurzinA.Nikitenko102103S.ObraztsovV.OreshkinV.PalichikV.PerelyginM.PerfilovS.Polikarpov99V.PopovO.Radchenko99M.SavinaV.SavrinV.ShalaevS.ShmatovS.ShulhaY.Skovpen99S.SlabospitskiiV.SmirnovD.SosnovV.SulimovE.TcherniaevA.TerkulovO.TeryaevI.TlisovaA.ToropinL.UvarovA.UzunianP.VolkovA.Vorobyev†G.VorotnikovN.VoytishinB.S.Yuldashev104A.ZarubinI.ZhizhinA.ZhokinAuthors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERNAuthors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERNAuthors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN99Also at another institute or international laboratory covered by a cooperation agreement with CERN.100Also at Universiteit Antwerpen, Antwerpen, Belgium.101Also at Northeastern University, Boston, Massachusetts, USA.102Also at Imperial College, London, United Kingdom.103Now at Yerevan Physics Institute, Yerevan, Armenia.104Also at Institute of Nuclear Physics of the Uzbekistan Academy of Sciences, Tashkent, Uzbekistan.CERN, Geneva, SwitzerlandCERNGenevaSwitzerlandCERN, Geneva, Switzerland⋆E-mail address:cms-publication-committee-chair@cern.ch.Editor: M. DoserAbstractA search is presented for new Higgs bosons in proton-proton (pp) collision events in which a same-sign top quark pair is produced in association with a jet, via the pp→tH/A→ttc‾ and pp→tH/A→ttu‾ processes. Here, H and A represent the extra scalar and pseudoscalar boson, respectively, of the second Higgs doublet in the generalized two-Higgs-doublet model (g2HDM). The search is based on pp collision data collected at a center-of-mass energy of 13 TeV with the CMS detector at the LHC, corresponding to an integrated luminosity of 138fb−1. Final states with a same-sign lepton pair in association with jets and missing transverse momentum are considered. New Higgs bosons in the 200–1000 GeV mass range and new Yukawa couplings between 0.1 and 1.0 are targeted in the search, for scenarios in which either H or A appear alone, or in which they coexist and interfere. No significant excess above the standard model prediction is observed. Exclusion limits are derived in the context of the g2HDM.KeywordsCMSTop quarksExtra Higgs bosonYukawa couplingsData availabilityRelease and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS policy as stated in “CMS data preservation, re-use and open access policy”.1IntroductionUsing proton-proton (pp) collision data recorded during the CERN LHC Run 1 (2011–2012) data-taking period, the ATLAS and CMS experiments discovered a scalar boson, h125, with a mass of 125 GeV, the properties of which are so far consistent with those of the Higgs boson of the standard model (SM) [1–3]. The analysis of the additional Run 2 (2015–2018) data enabled more precise measurements of the Higgs boson properties and further constrained the possible contributions from new physics beyond the SM [4,5]. The ATLAS and CMS experiments have measured the Yukawa couplings of the h125 boson to the t and b quarks, and the τ and μ leptons [6,7]. In all cases, the couplings are found to be consistent with the SM expectations within uncertainties.Having established the existence of one scalar SU(2) doublet, natural questions emerge about the possibility of additional doublets. A second doublet is predicted in two-Higgs-doublet models (2HDM), resulting in five physical scalar bosons: CP-even neutral scalar bosons h and H with mH>mh, a CP-odd pseudoscalar boson A, and two charged Higgs bosons H±[8]. These additional Higgs bosons at mass scales ≲1TeV may still exist within the reach of the LHC [9], but their signatures may be suppressed by fermion mass-mixing hierarchy [10] or alignment mechanisms, where the mixing angle γ between the two CP-even scalar bosons h and H has a value for which cos⁡γ≈0[11]. In the alignment limit [12–14], the lightest scalar boson h becomes the SM h125 boson, and the extra spin-0 bosons do not interact with vector boson pairs (i.e., HVV and AVV interactions do not occur, where V is a W or Z boson). Alignment suppresses flavor changing neutral current interactions of the h boson but allows them for the H and A bosons. Therefore, the lack of a hint of the processes such as t→ch125/uh125 or h125→μτ/eτ at the LHC may be because their amplitudes are suppressed by alignment. As shown in Ref. [11], the alignment scenario may occur if all extra Higgs quartic couplings are O(1) and no Z2 symmetry requirement is imposed, allowing flavor changing neutral Higgs couplings involving H and A bosons. This scenario without Z2 symmetry can be studied in the framework of the generalized 2HDM (g2HDM) [8,10,15], with new Yukawa couplings such as ρτμ, ρtu, ρtc, and ρtt that may assume significantly large values [8,10,15]. These new Yukawa couplings combined with Higgs quartic couplings of ≈1 may also explain the electroweak baryogenesis [16,17] and therefore the disappearance of antimatter soon after the Big Bang. The new top Yukawa coupling ρtc with a similar strength to ρτμ may be compatible with the observed data depending on the H± mass, which may also explain a possible muon g−2 anomaly [18]. These arguments strongly motivate to verify with direct experimental searches whether new Yukawa couplings exist. The processes discussed above have been recently explored by the ATLAS experiment [19].In this Letter, we present a search for the existence of the real part of these couplings, ρtu and ρtc, through the pp→tH/A→ttq‾(q=u,c) and the charge conjugate processes, considering one coupling at a time and keeping the other at zero using the Run 2 data set recorded by the CMS experiment. A representative Feynman diagram for the ttq‾ process is displayed in Fig. 1. The final-state signature for ttq‾ explored in this Letter consists of two same-sign (SS) leptons with at least three jets, two of which are identified as b jets and one compatible with originating from a u or c quark, and missing transverse momentum. The main background consists of events with nonprompt leptons originating from leptonic decays of heavy quarks, hadrons misidentified as leptons, electrons from photon conversions, or jets misidentified as leptons.The analysis is performed using pp collision data at a center-of-mass energy of 13 TeV. The data were collected with the CMS detector at the LHC between 2016 and 2018, and correspond to an integrated luminosity of 138fb−1. Tabulated results are accessible from the HEPData record for this analysis [20].The Letter is organized as follows: Section 2 describes the CMS detector, along with object reconstruction. In Section 3, a description of the simulation samples used in the analysis is given. The event selection and reconstruction procedure of the physics objects are given in Section 4. Following, in Section 5, the signal extraction procedure is explained. Section 6 discusses the sources of systematic uncertainties. The results of the analysis are presented in Section 7. Finally, a summary of the analysis is given in Section 8.2The CMS detector and object reconstructionThe CMS apparatus [21] is a multipurpose, nearly hermetic detector, designed to trigger on [22,23] and identify electrons, muons, photons, and (charged and neutral) hadrons [24–26]. A global “particle-flow” (PF) algorithm [27] aims to reconstruct all individual particles in an event, combining information provided by the all-silicon inner tracker and by the crystal electromagnetic (ECAL) and brass-scintillator hadron calorimeters (HCAL), operating inside a 3.8 T superconducting solenoid, with data from the gas-ionization muon detectors embedded in the flux-return yoke outside the solenoid.The primary vertex is taken to be the vertex corresponding to the hardest scattering in the event, evaluated using tracking information alone, as described in Section 9.4.1 of Ref. [28]. The energy of photons is obtained from the ECAL measurement. The energy of electrons is determined from a combination of the electron momentum at the primary interaction vertex as determined by the tracker, the energy of the corresponding ECAL cluster, and the energy sum of all bremsstrahlung photons spatially compatible with originating from the electron track. The energy of muons is obtained from the curvature of the corresponding track. The energy of charged hadrons is determined from a combination of their momentum measured in the tracker and the matching ECAL and HCAL energy deposits, corrected for the response function of the calorimeters to hadronic showers. Finally, the energy of neutral hadrons is obtained from the corresponding corrected ECAL and HCAL energies.Jets are built from PF particles using the anti-kT algorithm [29,30] with a distance parameter of 0.4. Jet momentum is determined as the vectorial sum of all particle momenta in the jet, and is found from simulation to be, on average, within 5 to 10% of the true momentum over the whole pT spectrum and detector acceptance. Additional pp interactions within the same or nearby bunch crossings can contribute additional tracks and calorimetric energy depositions, increasing the apparent jet momentum. To mitigate this effect, tracks identified to be originating from the multiple pp interactions occurring in the same or nearby bunch crossings (pileup) are discarded and an offset correction is applied to correct for remaining contributions [31]. Jet energy corrections are derived from simulation studies so that the average measured energy of jets becomes identical to that of particle level jets. In situ measurements of the momentum balance in dijet, photon+jet, Z+jets, and multijet events are used to determine any residual differences between the jet energy scale in data and in simulation, and appropriate corrections are made [32]. Additional selection criteria are applied to each jet to remove jets potentially dominated by instrumental effects or reconstruction failures [31]. The missing transverse momentum vector p→Tmiss is computed as the negative vector sum of the transverse momenta of all the PF candidates in an event, and its magnitude is denoted as pTmiss[33]. The p→Tmiss is modified to account for corrections to the energy scale of the reconstructed jets in the event.Events of interest are selected using a two-tiered trigger system. The first level (L1), composed of custom hardware processors, uses information from the calorimeters and muon detectors to select events at a rate of around 100 kHz within a fixed latency of about 4μs[22]. The second level, known as the high-level trigger, consists of a farm of processors running a version of the full event reconstruction software optimized for fast processing, and reduces the event rate to around 1 kHz before data storage [23].3Simulated event samplesThe signal and background processes are simulated using several Monte Carlo (MC) programs. The ttq‾ signal samples are simulated at leading order (LO) in perturbative quantum chromodynamics (QCD) with up to two additional noncollinear high-pT partons using MadGraph5_amc@nlo 2.6.5 [34], and the hard-process simulation is interfaced with parton shower jets using the MLM [35] matching prescription. Different signal samples are simulated for the case where a mass between 200 and 1000 GeV is assumed for A (H), and a mass too high to be of reach for our search is assumed for H (A). For these signal samples, there is no interference between A and H. Signal samples are also generated for the case where both A and H coexist and interfere assuming a mass difference mA−mH=50GeV, following Ref. [36]. The amplitudes for the processes qg→tA→ttq‾ and qg→tH→ttq‾ cancel when A and H are mass degenerate. The signal cross section is not significantly modified with respect to the noninterference case when the mass differences are larger than ≈100GeV. Therefore, the investigated mass difference is chosen to retain some interference effects along with reasonably high cross sections. Depending on the coupling value and the interference assumption we consider in this Letter, the cross sections for the ttu‾ process range from ≈1×10−4 to ≈7×10−1pb and for ttc‾ range from ≈5×10−6 to ≈7×10−2pb, as calculated with MadGraph5_amc@nlo at LO precision in QCD. The inclusive cross section for the ttq‾ process does not change, within uncertainties, when the intermediary particle is H or A, when there is no A-H interference.Background events generated by the MadGraph5_amc@nlo generator are tt‾V, V+jets, tt‾VV, tt‾VH, tZ, tt‾tj, tt‾tW, tt‾tt‾, WZ, vector boson scattering (VBS, i.e., Wℓℓqq or V±V±JJ), VVV, and single top quark s-channel production. Among these processes, FxFx matching [37] is used for tt‾W, Z+jets, and the QCD part of WZ production, while MLM matching [35] is used for W+jets. The powheg 2.0 generator [38–40] is used to simulate events at next-to-LO in perturbative QCD for tt‾[41], ZZ and W±W∓[42], single top quark tW [43] and t-channel [44], and tt‾H production [45].Both the signal and background samples are interfaced with pythia v8.240 [46] for parton showering, fragmentation, and hadronization. The underlying event is also modeled with pythia, using the CP5 tune [47]. The parton distribution functions (PDFs) are taken from the NNPDF3.1 next-to-next-to-LO set [48]. Finally, for both signal and background MC event samples, the detector response is modeled with the Geant4 package [49]. The simulated events are weighted to match the observables sensitive to pileup to those observed in the data [31].The simulated events are corrected for the differences between data and simulation of the trigger efficiencies, lepton identification, and lepton isolation. The corrections are determined using the “tag-and-probe” method applied on Z boson candidate events [50] and are parametrized as functions of the lepton pT and pseudorapidity (η).4Event reconstruction and selectionData are selected online with a combination of double lepton triggers and single lepton triggers to enhance signal efficiency. Charged leptons (electrons or muons) are required to originate from the primary vertex to reject contributions from pileup. Identification of electrons makes use of a multivariate discriminant [51,52] combining observables sensitive to the matching of charged-particle tracks in the tracker to the energy deposits in the ECAL and the amount of bremsstrahlung photons emitted along their trajectory [24]. The number of electrons originating from asymmetric photon conversions is reduced by requiring that their associated track has no missing hits in the innermost layers of the silicon tracker. To ensure the correct assignment of the electric charge of the electrons, further selection criteria were applied [53]. The separation of prompt leptons from nonprompt leptons reconstructed within jets is achieved by using an isolation variable, relative to the lepton pT. The isolation variable is constructed from the scalar pT sum of charged hadrons, neutral hadrons, and photons reconstructed within a cone of variable size that depends on the lepton pT[54]. “Loose” leptons are those that pass the kinematic selection criteria of pT>10GeV and |η|<2.5(2.4) for electrons (muons). Electrons that fall in the region between the ECAL barrel and endcaps (1.442<|η|<1.556) are vetoed. “Tight” leptons are in addition required to have pT>20GeV. A multivariate discriminant is furthermore used to separate prompt leptons and nonprompt leptons originating from the decays of hadrons inside jets, hadrons misidentified as leptons, and electrons from photon conversions. The jets must have pT>30GeV and |η|<2.4 to be considered. In addition, they are required to be separated from identified leptons by ΔR=(Δη)2+(Δϕ)2>0.4, where ϕ is the azimuthal angle measured in radians. At least three jets, and pTmiss>30GeV are required in each event. Jets from the hadronization of b quarks (b jets), c quarks (c jets), and light (i.e., light-quark or gluon) jets are distinguished through the ratios of the corresponding jet flavor probabilities, defined as CvsL (c vs light quark) and CvsB (c vs b quark) [55,56], respectively. These probabilities are obtained from the DeepJet[57,58] algorithm: a neural network utilizing global variables, charged, neutral particle and secondary vertex features in a jet to perform flavor tagging. The differences of the shapes of the CvsL and CvsB discriminant distributions between data and simulation are corrected by flavor-dependent scale factors.The search is performed in three SS dilepton categories: e±e±, μ±μ±, and e±μ±. The event selection ensures complete orthogonality of these three categories to avoid any possible double counting of events selected in the analysis. Events are required to have two tight leptons with the same electric charge for which the leading lepton has pT>30GeV and subleading lepton pT>20GeV. Events containing a third lepton are vetoed if the additional lepton passes the loose selection. The two leptons are required to be separated by ΔR(ℓ1,ℓ2)>0.3 and required to have an invariant mass m(ℓ1,ℓ2)>20GeV. Events with 60<m(ℓ1,ℓ2)<120GeV in the e±e± channel are vetoed to suppress the Drell-Yan (DY) background contribution, the main source of charge misidentified leptons. This veto reduces the selected number of DY events in simulation by about 94% after the aforementioned requirements. This veto is not applied to the e±μ± and μ±μ± channels, as the charge misidentification rate for muons is negligible. The CvsL and CvsB distributions for the leading jet obtained from simulated events and data are displayed in Fig. 2.The nonprompt-lepton background is estimated from control regions in the data using the fake-factor method [59]. A dijet enriched sample is selected from data, from which the probability fp for a loose nonprompt lepton (originating from a jet) to also pass the tight lepton selection criteria is estimated in bins of pT and |η|. The nonprompt-lepton background contribution is then estimated by applying fp to events in a data control sample in which at least one lepton fails the tight lepton selection criteria. A data-driven approach is followed to evaluate the lepton charge misidentification rate in the e±e± channel using DY events with same- and opposite-sign electric charges. It is estimated in bins of lepton pT and η, and is used to calibrate simulated events. The rate, which increases with pT and η, varies from ≈10−5 to ≈10−2.5Signal extractionA boosted decision tree (BDT) discriminant [60] is used to separate signal and background events. We train the BDT model in the signal region, where process yields of both backgrounds and signal are small. For the training, we combine the inputs from different channels. By comparing the BDT output distributions for the training and test samples, we found no evidence of overtraining. We use an optimized set of input observables, listed in Table 1, for our signal topology. Flavor tagging variables are used to differentiate b quarks originating from the top quark decay, and to differentiate c quark and light-quark jets. Pairwise kinematic variables related to jets are incorporated that are sensitive to the resonance structures, specifically to top quarks and A/H. Other kinematic features, such as HT and pTmiss, are also sensitive to our signal and are included. To mitigate the impact of resonances such as the DY process, the dilepton (+jets) invariant mass is also used as an input to the BDT.We use half of the available simulated events for the BDT training. The main backgrounds in the signal region are tt‾ (fully leptonic decay of the top quark-antiquark pair where one lepton has a misidentified charge), nonprompt leptons (dominated by semileptonic tt‾ decay), tt‾W, and tt‾H. In the signal extraction, we use events from data to estimate the nonprompt-lepton background contribution, but we do not use these events for training. Instead, we use simulated samples of semileptonically decaying tt‾ events for the BDT training, to mimic the misidentified lepton in the nonprompt-lepton background. We do not include events from W+jets or single top quark simulation, due to a limited number of simulated events. The various backgrounds are added corresponding to their cross sections. The MC event samples used for the BDT training are ttc‾ or ttu‾ signal, semileptonic tt‾, dileptonic tt‾ (tt‾), tt‾V, VV, VVV, tt‾H, tt‾VH, tt‾VV, tt‾tj, tt‾tW, tt‾tt‾, and VBS. Three values for the couplings ρtu and ρtc, namely, 0.1, 0.4, and 1.0 are considered. For each coupling, ten mA points are considered: 200, 300, 350, 400, 500, 600, 700, 800, 900, and 1000 GeV. Using the same coupling assumptions, we also consider the more realistic case with the A-H interference assuming a fixed mass difference mA−mH=50GeV, with the following nine mA-mH combinations; 250-200, 300-250, 350-300, 400-350, 550-500, 700-650, 800-750, 900-850, and 1000-950 GeV. The signal extraction is performed using the shape of the BDT discriminant distributions. Because of the kinematic differences and different background compositions, the BDTs are trained independently for four data-taking periods, two in 2016, and one for each of the years 2017 and 2018; for each mass assumption, namely for each mA either with no H present or with A-H interference; and for ρtu=0.4 and ρtc=0.4. Therefore, a total of 152 BDTs are trained. The values of the BDT hyperparameters, as defined in the TMVA package [61], are chosen after scanning a range of values, avoiding overtraining, and requiring a high background rejection rate while maintaining a high signal efficiency. We use these same model parameters for all three years of data taking. The BDTs offer high background rejection, while simultaneously maintaining a high signal efficiency. For instance, when considering ρtc=0.4, and a signal efficiency of 96%, the background rejection rates for mA=200GeV and 1000GeV are 50% and 76%, respectively.The signal strength parameter, μ, is obtained using a simultaneous maximum likelihood fit [62], in analyses performed for three decay modes and for four different eras (i.e. 12 categories) for each signal mass-coupling assumption independently. It is defined as μ=σ/σtheory, where σtheory is the predicted ttq‾ production cross section in g2HDM calculated with MadGraph5_amc@nlo +pythia, and σ is the upper limit on the observed cross section. To ensure numerical stability, the bin width is chosen to have a high enough yield in each bin of the BDT distributions. The BDT distribution ranges from −1 to 1, but to reduce the impact on the fit of background-dominated regions, events are selected with a BDT score >−0.6. This requirement on the BDT score also helps to improve the stability of the fit and the corresponding fit uncertainties. Except for the dominant nonprompt-lepton background, the predicted yields and the shapes of the BDT distributions are taken directly from the simulation. When performing the maximum likelihood fit, individual templates are used for the VBS, VV, tt‾ (fully leptonic decays), tt‾H, tt‾W, and nonprompt-lepton background processes, while a combined template labeled others uses a combination of background processes, namely: DY, tt‾VV, tt‾VH, tt‾Z, tt‾tj, tt‾tW, tt‾tt‾, VVV, tZq, tW, and t‾W.6Systematic uncertaintiesSystematic uncertainties, arising from various sources, such as detector effects, theoretical uncertainties, and mismodeling, are evaluated and categorized in two main groups: experimental uncertainties and modeling uncertainties. Several effects modify the event yields or shapes of the measured distributions. The systematic uncertainties are modeled as nuisance parameters in the maximum likelihood estimation procedure used for determining the best fit signal strength μˆ. The nuisance parameters are allowed to modify the shape and normalization of the backgrounds and signal in the fit using the method in Ref. [62]. The chosen probability density function (pdf) used for the interpolation between nominal and systematic templates is dependent on whether the associated nuisance parameter can also affect the shape of the nominal template or not. Log-normal pdfs are used for nuisance parameters that only affect the distributions normalization, whereas Gaussian distributions are used for those that can affect the shape as well. Experimental uncertainties, where appropriate, and all modeling uncertainties are taken as correlated across years and channels. The effect of the limited number of simulated events is estimated using the Barlow–Beeston-lite method [63].The experimental uncertainties are those related to the integrated luminosity [64–66], pileup, L1 trigger inefficiency, nonprompt-lepton background estimation, jet energy scale and resolution, unclustered energy scale, lepton identification and trigger efficiencies, charge misidentification, muon momentum scale, and heavy-quark, light-quark and gluon jet identification. The dominant experimental uncertainty sources are related to the flavor tagger discriminant shape calibration, and nonprompt-lepton background estimation. The modeling uncertainty sources are matrix-element renormalization and factorization scales, parton shower scales that control the initial- and final-state radiation, and PDFs. For the signal, these are included as separate nuisance parameters that affect the shape. For the backgrounds estimated using MC event samples, nuisance parameters are assumed to only affect the yields, and the corresponding uncertainties in the theoretical cross section calculations are used. The most significant modeling uncertainty in the analysis is attributed to the normalization of the tt‾W background, regardless of the A-H interference. The contributions of all uncertainty sources on the pre-fit expected event yields are displayed in Table 2, for ρtc=0.4 and mA=350GeV with A-H interference assuming mA−mH=50GeV. The uncertainties in other scenarios are similar.7ResultsFig. 3 displays the post-fit BDT discriminant distributions used for the signal extraction combining the categories e±e±, μ±μ±, and e±μ±, and for ρtu=1.0 and ρtc=1.0 with A-H interference, assuming mA=350GeV.No significant excess over the expected SM background is observed. The results of the search are interpreted in terms of the upper limits on the signal strength parameter μ in the g2HDM. The upper limits on μ are calculated at 95% confidence level (CL) using a modified frequentist method [67–69] computed with an asymptotic approximation [70]. The expected 95% CL on the production cross section and the regions containing 68 and 95% of the distribution of the limits expected under the background-only hypothesis are calculated with pseudo-experiments using background-only samples. It is observed that the shapes of the BDT distributions are consistent with each other for different coupling values at the same A or H mass value. Therefore, for other coupling assumptions than ρtu/tc=0.4, the expected signal yields are scaled separately for ρtu and ρtc for each mass and coupling hypothesis making use of the corresponding signal cross sections. It is also observed that A or H can be used interchangeably as their corresponding BDT distribution shapes as well as their cross sections are the same. Therefore, we only show the results for A in this Letter. The observed and expected upper limits are displayed as functions of mA from 200 to 1000 GeV for ρtu=0.1,0.4,1.0 and ρtc=0.1,0.4,1.0, for the Run-2 data and for the combination of all three decay modes, without (with) A-H interference in Fig. 4(5). The observed limits at 95% CL on the signal strength as functions of mA and the new Yukawa couplings ρtc/tu are shown in Fig. 6 without A-H interference, and in Fig. 7 with A-H interference. Interpreted in g2HDM, exclusion limits at 95% CL on the mass of the additional Higgs bosons A and H are shown in Table 3 for different ρtu and ρtc assumptions.8SummaryA search for new Yukawa couplings of the top quark in models with additional Higgs bosons in proton-proton collisions at a center-of-mass energy of 13 TeV has been presented. The process considered is the production of same-sign top quark pairs associated with an up or a charm quark, and resulting in a final state containing two same-sign leptons and jets. No significant excess above the background prediction is observed. When no interference between the pseudoscalar (A) and scalar (H) Higgs bosons is assumed, A or H bosons with masses below 920 GeV and 1000 GeV are excluded at the 95% confidence level (CL) for coupling values ρtu=0.4 and 1.0, respectively, while all other extra Yukawa couplings are assumed to be zero. Similarly, without interference between H and A, and assuming a coupling value of ρtc=1.0, A or H bosons with masses below approximately 770GeV are excluded at the 95% CL. Under the assumption that A and H interfere in the scenario with a mass difference of mA−mH=50GeV, the pseudoscalar Higgs boson is excluded for mA values below 1000GeV when considering coupling values ρtu>0.4. Furthermore, assuming ρtc=0.4, the exclusion limit for A is mA=340GeV, whereas assuming ρtc=1.0, the limit extends to mA=810GeV at 95% CL. These results represent the first search based on the generalized two-Higgs-doublet model considering A-H interference.Declaration of Competing InterestThe authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.AcknowledgementsWe congratulate our colleagues in the CERN accelerator departments for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their contributions to the success of the CMS effort. In addition, we gratefully acknowledge the computing centers and personnel of the Worldwide LHC Computing Grid and other centers for delivering so effectively the computing infrastructure essential to our analyses. Finally, we acknowledge the enduring support for the construction and operation of the LHC, the CMS detector, and the supporting computing infrastructure provided by the following funding agencies: SC (Armenia), BMBWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, FAPERGS, and FAPESP (Brazil); MES and BNSF (Bulgaria); CERN; CAS, MOST, and NSFC (China); Minciencias (Colombia); MSES and CSF (Croatia); RIF (Cyprus); SENESCYT (Ecuador); MoER, ERC PUT and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); SRNSF (Georgia); BMBF, DFG, and HGF (Germany); GSRI (Greece); NKFIH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); MSIP and NRF (Republic of Korea); MES (Latvia); LAS (Lithuania); MOE and UM (Malaysia); BUAP, CINVESTAV, CONACYT, LNS, SEP, and UASLP-FAI (Mexico); MOS (Montenegro); MBIE (New Zealand); PAEC (Pakistan); MES and NSC (Poland); FCT (Portugal); MESTD (Serbia); MCIN/AEI and PCTI (Spain); MoSTR (Sri Lanka); Swiss Funding Agencies (Switzerland); MST (Taipei); MHESI and NSTDA (Thailand); TUBITAK and TENMAK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA).Individuals have received support from the Marie-Curie program and the European Research Council and Horizon 2020 Grant, contract Nos. 675440, 724704, 752730, 758316, 765710, 824093, and COST Action CA16108 (European Union); the Leventis Foundation; the Alfred P. Sloan Foundation; the Alexander von Humboldt Foundation; the Science Committee, project no. 22rl-037 (Armenia); the Belgian Federal Science Policy Office; the Fonds pour la Formation à la Recherche dans l'Industrie et dans l'Agriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); the F.R.S.-FNRS and FWO (Belgium) under the “Excellence of Science – EOS” – be.h project n. 30820817; the Beijing Municipal Science & Technology Commission, No. Z191100007219010 and Fundamental Research Funds for the Central Universities (China); The Ministry of Education, Youth and Sports (MEYS) of the Czech Republic; the Shota Rustaveli National Science Foundation, grant FR-22-985 (Georgia); the Deutsche Forschungsgemeinschaft (DFG), under Germany's Excellence Strategy – EXC 2121 “Quantum Universe” – 390833306, and under project number 400140256 - GRK2497; the Hellenic Foundation for Research and Innovation (HFRI), Project Number 2288 (Greece); the Hungarian Academy of Sciences, the New National Excellence Program - ÚNKP, the NKFIH research grants K 124845, K 124850, K 128713, K 128786, K 129058, K 131991, K 133046, K 138136, K 143460, K 143477, 2020-2.2.1-ED-2021-00181, and TKP2021-NKTA-64 (Hungary); the Council of Science and Industrial Research, India; ICSC – National Research Center for High Performance Computing, Big Data and Quantum Computing, funded by the EU NexGeneration program (Italy); the Latvian Council of Science; the Ministry of Education and Science, project no. 2022/WK/14, and the National Science Center, contracts Opus 2021/41/B/ST2/01369 and 2021/43/B/ST2/01552 (Poland); the Fundação para a Ciência e a Tecnologia, grant CEECIND/01334/2018 (Portugal); the National Priorities Research Program by Qatar National Research Fund; MCIN/AEI/10.13039/501100011033, ERDF “a way of making Europe”, and the Programa Estatal de Fomento de la Investigación Científica y Técnica de Excelencia María de Maeztu, grant MDM-2017-0765 and Programa Severo Ochoa del Principado de Asturias (Spain); the Chulalongkorn Academic into Its 2nd Century Project Advancement Project, and the National Science, Research and Innovation Fund via the Program Management Unit for Human Resources & Institutional Development, Research and Innovation, grant B05F650021 (Thailand); the Kavli Foundation; the Nvidia Corporation; the SuperMicro Corporation; the Welch Foundation, contract C-1845; and the Weston Havens Foundation (USA).References[1]ATLAS CollaborationObservation of a new particle in the search for the standard model Higgs boson with the ATLAS detector at the LHCPhys. 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Armenia." } @@ -125,6 +128,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institut f\u00fcr Hochenergiephysik, Vienna, Austria" + }, { "affPubRaw": "Also at TU Wien, Vienna, Austria." } @@ -195,6 +201,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institut f\u00fcr Hochenergiephysik, Vienna, Austria" + }, { "affPubRaw": "Also at TU Wien, Vienna, Austria." } @@ -279,6 +288,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institut f\u00fcr Hochenergiephysik, Vienna, Austria" + }, { "affPubRaw": "Also at TU Wien, Vienna, Austria." } @@ -293,6 +305,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Universiteit Antwerpen, Antwerpen, Belgium" + }, { "affPubRaw": "Also at Institute of Basic and Applied Sciences, Faculty of Engineering, Arab Academy for Science, Technology and Maritime Transport, Alexandria, Egypt." } @@ -489,6 +504,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Vrije Universiteit Brussel, Brussel, Belgium" + }, { "affPubRaw": "Also at Ghent University, Ghent, Belgium." } @@ -1263,6 +1281,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Universidade do Estado do Rio de Janeiro, Rio de Janeiro, Brazil" + }, { "affPubRaw": "Also at Universidade Estadual de Campinas, Campinas, Brazil." } @@ -1288,6 +1309,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Universidade do Estado do Rio de Janeiro, Rio de Janeiro, Brazil" + }, { "affPubRaw": "Also at Federal University of Rio Grande do Sul, Porto Alegre, Brazil." } @@ -1330,6 +1354,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Universidade do Estado do Rio de Janeiro, Rio de Janeiro, Brazil" + }, { "affPubRaw": "Also at UFMS, Nova Andradina, Brazil." } @@ -1455,6 +1482,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Universidade Estadual Paulista, Universidade Federal do ABC, S\u00e3o Paulo, Brazil" + } + ], "attrib": { "orcid": "0000-0001-5790-9563" }, @@ -1851,6 +1883,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Department of Physics, Tsinghua University, Beijing, China" + }, { "affPubRaw": "Also at Nanjing Normal University, Nanjing, China." } @@ -1865,6 +1900,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institute of High Energy Physics, Beijing, China" + }, { "affPubRaw": "Also at University of Chinese Academy of Sciences, Beijing, China." } @@ -1879,6 +1917,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institute of High Energy Physics, Beijing, China" + }, { "affPubRaw": "Also at University of Chinese Academy of Sciences, Beijing, China." } @@ -1893,6 +1934,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institute of High Energy Physics, Beijing, China" + }, { "affPubRaw": "Also at University of Chinese Academy of Sciences, Beijing, China." } @@ -1932,6 +1976,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institute of High Energy Physics, Beijing, China" + }, { "affPubRaw": "Also at China Center of Advanced Science and Technology, Beijing, China." } @@ -1960,6 +2007,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institute of High Energy Physics, Beijing, China" + }, { "affPubRaw": "Also at University of Chinese Academy of Sciences, Beijing, China." } @@ -1974,6 +2024,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institute of High Energy Physics, Beijing, China" + }, { "affPubRaw": "Also at China Spallation Neutron Source, Guangdong, China." } @@ -1988,6 +2041,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institute of High Energy Physics, Beijing, China" + }, { "affPubRaw": "Also at University of Chinese Academy of Sciences, Beijing, China." } @@ -2013,6 +2069,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institute of High Energy Physics, Beijing, China" + }, { "affPubRaw": "Also at University of Chinese Academy of Sciences, Beijing, China." } @@ -2038,6 +2097,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institute of High Energy Physics, Beijing, China" + }, { "affPubRaw": "Also at University of Chinese Academy of Sciences, Beijing, China." } @@ -2253,6 +2315,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Nanjing Normal University, Nanjing, China" + }, { "affPubRaw": "Now at Henan Normal University, Xinxiang, China." } @@ -2264,6 +2329,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institute of Modern Physics and Key Laboratory of Nuclear Physics and Ion-beam Application (MOE) - Fudan University, Shanghai, China" + }, { "affPubRaw": "Also at Universit\u00e9 Libre de Bruxelles, Bruxelles, Belgium." } @@ -2563,6 +2631,9 @@ }, { "affiliation": [ + { + "affPubRaw": "University of Split, Faculty of Science, Split, Croatia" + }, { "affPubRaw": "Also at University of Latvia (LU), Riga, Latvia." } @@ -2647,6 +2718,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institute Rudjer Boskovic, Zagreb, Croatia" + }, { "affPubRaw": "Also at an institute or an international laboratory covered by a cooperation agreement with CERN." } @@ -2879,6 +2953,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Academy of Scientific Research and Technology of the Arab Republic of Egypt, Egyptian Network of High Energy Physics, Cairo, Egypt" + }, { "affPubRaw": "Also at Cairo University, Cairo, Egypt." } @@ -2893,6 +2970,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Academy of Scientific Research and Technology of the Arab Republic of Egypt, Egyptian Network of High Energy Physics, Cairo, Egypt" + }, { "affPubRaw": "Also at Suez University, Suez, Egypt." } @@ -2932,6 +3012,9 @@ }, { "affiliation": [ + { + "affPubRaw": "National Institute of Chemical Physics and Biophysics, Tallinn, Estonia" + }, { "affPubRaw": "Also at Birla Institute of Technology, Mesra, Mesra, India." } @@ -3371,6 +3454,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Lappeenranta-Lahti University of Technology, Lappeenranta, Finland" + }, { "affPubRaw": "Deceased." } @@ -3569,6 +3655,9 @@ }, { "affiliation": [ + { + "affPubRaw": "IRFU, CEA, Universit\u00e9 Paris-Saclay, Gif-sur-Yvette, France" + }, { "affPubRaw": "Also at Purdue University, West Lafayette, Indiana, USA." } @@ -4031,6 +4120,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Universit\u00e9 de Strasbourg, CNRS, IPHC UMR 7178, Strasbourg, France" + }, { "affPubRaw": "Also at Universit\u00e9 de Haute Alsace, Mulhouse, France." } @@ -4350,6 +4442,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institut de Physique des 2 Infinis de Lyon (IP2I), Villeurbanne, France" + }, { "affPubRaw": "Also at Department of Physics, Tsinghua University, Beijing, China." } @@ -4558,6 +4653,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Georgian Technical University, Tbilisi, Georgia" + } + ], "attrib": { "orcid": "0000-0002-5953-0140" }, @@ -4581,6 +4681,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Georgian Technical University, Tbilisi, Georgia" + } + ], "attrib": { "orcid": "0000-0001-5377-3558" }, @@ -5139,6 +5244,9 @@ }, { "affiliation": [ + { + "affPubRaw": "RWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany" + }, { "affPubRaw": "Also at The University of the State of Amazonas, Manaus, Brazil." } @@ -5217,6 +5325,9 @@ }, { "affiliation": [ + { + "affPubRaw": "RWTH Aachen University, III. Physikalisches Institut B, Aachen, Germany" + }, { "affPubRaw": "Also at Erzincan Binali Yildirim University, Erzincan, Turkey." } @@ -5466,6 +5577,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Deutsches Elektronen-Synchrotron, Hamburg, Germany" + }, { "affPubRaw": "Also at University of Hamburg, Hamburg, Germany." } @@ -5480,6 +5594,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Deutsches Elektronen-Synchrotron, Hamburg, Germany" + }, { "affPubRaw": "Also at RWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany." } @@ -5656,6 +5773,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Deutsches Elektronen-Synchrotron, Hamburg, Germany" + }, { "affPubRaw": "Also at University of Hamburg, Hamburg, Germany." } @@ -5751,6 +5871,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Deutsches Elektronen-Synchrotron, Hamburg, Germany" + }, { "affPubRaw": "Also at Isfahan University of Technology, Isfahan, Iran." } @@ -5916,6 +6039,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Deutsches Elektronen-Synchrotron, Hamburg, Germany" + }, { "affPubRaw": "Also at Bergische University Wuppertal (BUW), Wuppertal, Germany." } @@ -5930,6 +6056,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Deutsches Elektronen-Synchrotron, Hamburg, Germany" + }, { "affPubRaw": "Also at Brandenburg University of Technology, Cottbus, Germany." } @@ -6173,6 +6302,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Deutsches Elektronen-Synchrotron, Hamburg, Germany" + }, { "affPubRaw": "Also at Forschungszentrum J\u00fclich, Juelich, Germany." } @@ -6187,6 +6319,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Deutsches Elektronen-Synchrotron, Hamburg, Germany" + }, { "affPubRaw": "Also at RWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany." } @@ -6215,6 +6350,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Deutsches Elektronen-Synchrotron, Hamburg, Germany" + }, { "affPubRaw": "Also at University of Hamburg, Hamburg, Germany." } @@ -6363,6 +6501,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Deutsches Elektronen-Synchrotron, Hamburg, Germany" + }, { "affPubRaw": "Also at RWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany." } @@ -7176,6 +7317,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Karlsruher Institut fuer Technologie, Karlsruhe, Germany" + }, { "affPubRaw": "Also at CERN, European Organization for Nuclear Research, Geneva, Switzerland." } @@ -7492,6 +7636,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Karlsruher Institut fuer Technologie, Karlsruhe, Germany" + }, { "affPubRaw": "Now at an institute or an international laboratory covered by a cooperation agreement with CERN." } @@ -7661,6 +7808,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Institute of Nuclear and Particle Physics (INPP), NCSR Demokritos, Aghia Paraskevi, Greece" + } + ], "name": { "given_name": "A.", "surname": "Papadopoulos" @@ -8069,6 +8221,9 @@ }, { "affiliation": [ + { + "affPubRaw": "HUN-REN Wigner Research Centre for Physics, Budapest, Hungary" + }, { "affPubRaw": "Also at Institute of Physics, University of Debrecen, Debrecen, Hungary." } @@ -8097,6 +8252,9 @@ }, { "affiliation": [ + { + "affPubRaw": "HUN-REN Wigner Research Centre for Physics, Budapest, Hungary" + }, { "affPubRaw": "Also at Institute of Nuclear Research ATOMKI, Debrecen, Hungary." } @@ -8167,6 +8325,9 @@ }, { "affiliation": [ + { + "affPubRaw": "MTA-ELTE Lend\u00fclet CMS Particle and Nuclear Physics Group, E\u00f6tv\u00f6s Lor\u00e1nd University, Budapest, Hungary" + }, { "affPubRaw": "Also at Physics Department, Faculty of Science, Assiut University, Assiut, Egypt." } @@ -8237,6 +8398,9 @@ }, { "affiliation": [ + { + "affPubRaw": "MTA-ELTE Lend\u00fclet CMS Particle and Nuclear Physics Group, E\u00f6tv\u00f6s Lor\u00e1nd University, Budapest, Hungary" + }, { "affPubRaw": "Also at HUN-REN Wigner Research Centre for Physics, Budapest, Hungary." } @@ -8325,6 +8489,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Institute of Nuclear Research ATOMKI, Debrecen, Hungary" + } + ], "attrib": { "orcid": "0000-0003-0802-7665" }, @@ -8356,6 +8525,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Karoly Robert Campus, MATE Institute of Technology, Gyongyos, Hungary" + } + ], "attrib": { "orcid": "0000-0002-9110-9663" }, @@ -8365,6 +8539,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Karoly Robert Campus, MATE Institute of Technology, Gyongyos, Hungary" + } + ], "attrib": { "orcid": "0000-0002-1451-6484" }, @@ -8470,6 +8649,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Panjab University, Chandigarh, India" + }, { "affPubRaw": "Also at Punjab Agricultural University, Ludhiana, India." } @@ -8747,6 +8929,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Saha Institute of Nuclear Physics, HBNI, Kolkata, India" + }, { "affPubRaw": "Also at University of Visva-Bharati, Santiniketan, India." } @@ -8909,6 +9094,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Indian Institute of Technology Madras, Madras, India" + }, { "affPubRaw": "Also at Indian Institute of Science (IISc), Bangalore, India." } @@ -8923,6 +9111,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Indian Institute of Technology Madras, Madras, India" + }, { "affPubRaw": "Also at Indian Institute of Science (IISc), Bangalore, India." } @@ -8937,6 +9128,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Indian Institute of Technology Madras, Madras, India" + }, { "affPubRaw": "Also at Indian Institute of Science (IISc), Bangalore, India." } @@ -9222,6 +9416,9 @@ }, { "affiliation": [ + { + "affPubRaw": "National Institute of Science Education and Research, An OCC of Homi Bhabha National Institute, Bhubaneswar, Odisha, India" + }, { "affPubRaw": "Also at IIT Bhubaneswar, Bhubaneswar, India." } @@ -9261,6 +9458,9 @@ }, { "affiliation": [ + { + "affPubRaw": "National Institute of Science Education and Research, An OCC of Homi Bhabha National Institute, Bhubaneswar, Odisha, India" + }, { "affPubRaw": "Also at Institute of Physics, Bhubaneswar, India." } @@ -9303,6 +9503,9 @@ }, { "affiliation": [ + { + "affPubRaw": "National Institute of Science Education and Research, An OCC of Homi Bhabha National Institute, Bhubaneswar, Odisha, India" + }, { "affPubRaw": "Also at Institute of Physics, Bhubaneswar, India." } @@ -9317,6 +9520,9 @@ }, { "affiliation": [ + { + "affPubRaw": "National Institute of Science Education and Research, An OCC of Homi Bhabha National Institute, Bhubaneswar, Odisha, India" + }, { "affPubRaw": "Also at Institute of Physics, Bhubaneswar, India." } @@ -9331,6 +9537,9 @@ }, { "affiliation": [ + { + "affPubRaw": "National Institute of Science Education and Research, An OCC of Homi Bhabha National Institute, Bhubaneswar, Odisha, India" + }, { "affPubRaw": "Also at Institute of Physics, Bhubaneswar, India." } @@ -9384,6 +9593,9 @@ }, { "affiliation": [ + { + "affPubRaw": "National Institute of Science Education and Research, An OCC of Homi Bhabha National Institute, Bhubaneswar, Odisha, India" + }, { "affPubRaw": "Also at Institute of Physics, Bhubaneswar, India." } @@ -9398,6 +9610,9 @@ }, { "affiliation": [ + { + "affPubRaw": "National Institute of Science Education and Research, An OCC of Homi Bhabha National Institute, Bhubaneswar, Odisha, India" + }, { "affPubRaw": "Also at Institute of Physics, Bhubaneswar, India." } @@ -9412,6 +9627,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Indian Institute of Science Education and Research (IISER), Pune, India" + }, { "affPubRaw": "Also at University of Hyderabad, Hyderabad, India." } @@ -9454,6 +9672,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Indian Institute of Science Education and Research (IISER), Pune, India" + }, { "affPubRaw": "Also at University of Hyderabad, Hyderabad, India." } @@ -9496,6 +9717,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Indian Institute of Science Education and Research (IISER), Pune, India" + }, { "affPubRaw": "Also at University of Hyderabad, Hyderabad, India." } @@ -9524,6 +9748,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Isfahan University of Technology, Isfahan, Iran" + }, { "affPubRaw": "Also at Deutsches Elektronen-Synchrotron, Hamburg, Germany." } @@ -9538,6 +9765,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Isfahan University of Technology, Isfahan, Iran" + }, { "affPubRaw": "Also at Department of Physics, Isfahan University of Technology, Isfahan, Iran." } @@ -9552,6 +9782,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Isfahan University of Technology, Isfahan, Iran" + }, { "affPubRaw": "Also at Sharif University of Technology, Tehran, Iran." } @@ -9566,6 +9799,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Institute for Research in Fundamental Sciences (IPM), Tehran, Iran" + }, { "affPubRaw": "Also at Department of Physics, University of Science and Technology of Mazandaran, Behshahr, Iran." } @@ -10814,6 +11050,9 @@ }, { "affiliation": [ + { + "affPubRaw": "INFN Laboratori Nazionali di Frascati, Frascati, Italy" + }, { "affPubRaw": "Also at Universit\u00e0 degli Studi Guglielmo Marconi, Roma, Italy." } @@ -14413,6 +14652,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Riga Technical University, Riga, Latvia" + }, { "affPubRaw": "Also at Riga Technical University, Riga, Latvia." } @@ -14511,6 +14753,9 @@ }, { "affiliation": [ + { + "affPubRaw": "National Centre for Particle Physics, Universiti Malaya, Kuala Lumpur, Malaysia" + }, { "affPubRaw": "Also at Department of Applied Physics, Faculty of Science and Technology, Universiti Kebangsaan Malaysia, Bangi, Malaysia." } @@ -14684,6 +14929,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Centro de Investigacion y de Estudios Avanzados del IPN, Mexico City, Mexico" + }, { "affPubRaw": "Also at Consejo Nacional de Ciencia y Tecnolog\u00eda, Mexico City, Mexico." } @@ -16362,6 +16610,9 @@ }, { "affiliation": [ + { + "affPubRaw": "University of Colombo, Colombo, Sri Lanka" + }, { "affPubRaw": "Also at Trincomalee Campus, Eastern University, Sri Lanka, Nilaveli, Sri Lanka." } @@ -16404,6 +16655,9 @@ }, { "affiliation": [ + { + "affPubRaw": "University of Ruhuna, Department of Physics, Matara, Sri Lanka" + }, { "affPubRaw": "Also at Saegis Campus, Nugegoda, Sri Lanka." } @@ -16765,6 +17019,9 @@ }, { "affiliation": [ + { + "affPubRaw": "CERN, European Organization for Nuclear Research, Geneva, Switzerland" + }, { "affPubRaw": "Also at INFN Sezione di Pavia, Universit\u00e0 di Pavia, Pavia, Italy." } @@ -17427,6 +17684,9 @@ }, { "affiliation": [ + { + "affPubRaw": "CERN, European Organization for Nuclear Research, Geneva, Switzerland" + }, { "affPubRaw": "Also at National and Kapodistrian University of Athens, Athens, Greece." } @@ -17536,6 +17796,9 @@ }, { "affiliation": [ + { + "affPubRaw": "CERN, European Organization for Nuclear Research, Geneva, Switzerland" + }, { "affPubRaw": "Also at Ecole Polytechnique F\u00e9d\u00e9rale Lausanne, Lausanne, Switzerland." } @@ -17614,6 +17877,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Paul Scherrer Institut, Villigen, Switzerland" + }, { "affPubRaw": "Also at Universit\u00e4t Z\u00fcrich, Zurich, Switzerland." } @@ -17628,6 +17894,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Paul Scherrer Institut, Villigen, Switzerland" + }, { "affPubRaw": "Also at Universit\u00e4t Z\u00fcrich, Zurich, Switzerland." } @@ -17740,6 +18009,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Paul Scherrer Institut, Villigen, Switzerland" + }, { "affPubRaw": "Also at Universit\u00e4t Z\u00fcrich, Zurich, Switzerland." } @@ -17754,6 +18026,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Paul Scherrer Institut, Villigen, Switzerland" + }, { "affPubRaw": "Also at Universit\u00e4t Z\u00fcrich, Zurich, Switzerland." } @@ -17795,6 +18070,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "ETH Zurich - Institute for Particle Physics and Astrophysics (IPA), Zurich, Switzerland" + } + ], "attrib": { "orcid": "0000-0003-2694-6542" }, @@ -18081,6 +18361,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "ETH Zurich - Institute for Particle Physics and Astrophysics (IPA), Zurich, Switzerland" + } + ], "attrib": { "orcid": "0000-0001-6362-5356" }, @@ -18255,6 +18540,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "ETH Zurich - Institute for Particle Physics and Astrophysics (IPA), Zurich, Switzerland" + } + ], "attrib": { "orcid": "0000-0003-4420-5510" }, @@ -18293,6 +18583,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Universit\u00e4t Z\u00fcrich, Zurich, Switzerland" + }, { "affPubRaw": "Also at Stefan Meyer Institute for Subatomic Physics, Vienna, Austria." } @@ -18634,6 +18927,9 @@ }, { "affiliation": [ + { + "affPubRaw": "National Central University, Chung-Li, Taiwan" + }, { "affPubRaw": "Also at Laboratoire d'Annecy-le-Vieux de Physique des Particules, IN2P3-CNRS, Annecy-le-Vieux, France." } @@ -18691,6 +18987,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "National Central University, Chung-Li, Taiwan" + } + ], "attrib": { "orcid": "0000-0002-3667-3843" }, @@ -19038,6 +19339,9 @@ }, { "affiliation": [ + { + "affPubRaw": "\u00c7ukurova University, Physics Department, Science and Art Faculty, Adana, Turkey" + }, { "affPubRaw": "Also at Near East University, Research Center of Experimental Health Science, Mersin, Turkey." } @@ -19066,6 +19370,9 @@ }, { "affiliation": [ + { + "affPubRaw": "\u00c7ukurova University, Physics Department, Science and Art Faculty, Adana, Turkey" + }, { "affPubRaw": "Also at Konya Technical University, Konya, Turkey." } @@ -19080,6 +19387,9 @@ }, { "affiliation": [ + { + "affPubRaw": "\u00c7ukurova University, Physics Department, Science and Art Faculty, Adana, Turkey" + }, { "affPubRaw": "Also at Konya Technical University, Konya, Turkey." } @@ -19161,6 +19471,9 @@ }, { "affiliation": [ + { + "affPubRaw": "\u00c7ukurova University, Physics Department, Science and Art Faculty, Adana, Turkey" + }, { "affPubRaw": "Also at Izmir Bakircay University, Izmir, Turkey." } @@ -19189,6 +19502,9 @@ }, { "affiliation": [ + { + "affPubRaw": "\u00c7ukurova University, Physics Department, Science and Art Faculty, Adana, Turkey" + }, { "affPubRaw": "Also at Adiyaman University, Adiyaman, Turkey." } @@ -19259,6 +19575,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Middle East Technical University, Physics Department, Ankara, Turkey" + }, { "affPubRaw": "Also at Bozok Universitetesi Rekt\u00f6rl\u00fcg\u00fc, Yozgat, Turkey." } @@ -19315,6 +19634,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Bogazici University, Istanbul, Turkey" + }, { "affPubRaw": "Also at Marmara University, Istanbul, Turkey." } @@ -19329,6 +19651,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Bogazici University, Istanbul, Turkey" + }, { "affPubRaw": "Also at Milli Savunma University, Istanbul, Turkey." } @@ -19343,6 +19668,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Bogazici University, Istanbul, Turkey" + }, { "affPubRaw": "Also at Kafkas University, Kars, Turkey." } @@ -19370,6 +19698,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Istanbul Technical University, Istanbul, Turkey" + } + ], "attrib": { "orcid": "0000-0002-3829-3481" }, @@ -19394,6 +19727,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Istanbul Technical University, Istanbul, Turkey" + }, { "affPubRaw": "Also at Hacettepe University, Ankara, Turkey." } @@ -19421,6 +19757,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Istanbul University, Istanbul, Turkey" + } + ], "attrib": { "orcid": "0000-0002-8702-6152" }, @@ -19459,6 +19800,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Istanbul University, Istanbul, Turkey" + }, { "affPubRaw": "Also at Istanbul University - Cerrahpasa, Faculty of Engineering, Istanbul, Turkey." } @@ -19542,6 +19886,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Istanbul University, Istanbul, Turkey" + } + ], "attrib": { "orcid": "0000-0002-5412-4688" }, @@ -19566,6 +19915,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Yildiz Technical University, Istanbul, Turkey" + }, { "affPubRaw": "Also at Yildiz Technical University, Istanbul, Turkey." } @@ -19812,6 +20164,9 @@ }, { "affiliation": [ + { + "affPubRaw": "University of Bristol, Bristol, United Kingdom" + }, { "affPubRaw": "Also at Vrije Universiteit Brussel, Brussel, Belgium." } @@ -19876,6 +20231,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Rutherford Appleton Laboratory, Didcot, United Kingdom" + }, { "affPubRaw": "Also at School of Physics and Astronomy, University of Southampton, Southampton, United Kingdom." } @@ -19985,6 +20343,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Rutherford Appleton Laboratory, Didcot, United Kingdom" + }, { "affPubRaw": "Also at University of Bristol, Bristol, United Kingdom." } @@ -20222,6 +20583,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Imperial College, London, United Kingdom" + }, { "affPubRaw": "Also at IPPP Durham University, Durham, United Kingdom." } @@ -20515,6 +20879,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Imperial College, London, United Kingdom" + }, { "affPubRaw": "Also at Monash University, Faculty of Science, Clayton, Australia." } @@ -20659,6 +21026,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Imperial College, London, United Kingdom" + } + ], "attrib": { "orcid": "0000-0001-7429-2198" }, @@ -21080,6 +21452,9 @@ }, { "affiliation": [ + { + "affPubRaw": "The University of Alabama, Tuscaloosa, AL, USA" + }, { "affPubRaw": "Also at Universit\u00e0 di Torino, Torino, Italy." } @@ -21429,6 +21804,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Brown University, Providence, RI, USA" + } + ], "name": { "given_name": "X.", "surname": "Coubez" @@ -21478,6 +21858,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Brown University, Providence, RI, USA" + }, { "affPubRaw": "Also at Bethel University, St. Paul, Minnesota, USA." } @@ -21575,6 +21958,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Brown University, Providence, RI, USA" + } + ], "attrib": { "orcid": "0000-0002-7857-7403" }, @@ -21599,6 +21987,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Brown University, Providence, RI, USA" + }, { "affPubRaw": "Also at Karamano\u011flu Mehmetbey University, Karaman, Turkey." } @@ -22157,6 +22548,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "University of California, Riverside, Riverside, CA, USA" + } + ], "attrib": { "orcid": "0000-0003-0505-4908" }, @@ -24319,6 +24715,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Fermi National Accelerator Laboratory, Batavia, IL, USA" + }, { "affPubRaw": "Also at California Institute of Technology, Pasadena, California, USA." } @@ -24347,6 +24746,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Fermi National Accelerator Laboratory, Batavia, IL, USA" + }, { "affPubRaw": "Also at United States Naval Academy, Annapolis, Maryland, USA." } @@ -25112,6 +25514,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Florida Institute of Technology, Melbourne, FL, USA" + } + ], "attrib": { "orcid": "0000-0001-9930-6445" }, @@ -25544,6 +25951,9 @@ }, { "affiliation": [ + { + "affPubRaw": "The University of Iowa, Iowa City, IA, USA" + }, { "affPubRaw": "Also at Bingol University, Bingol, Turkey." } @@ -25611,6 +26021,9 @@ }, { "affiliation": [ + { + "affPubRaw": "The University of Iowa, Iowa City, IA, USA" + }, { "affPubRaw": "Also at Georgian Technical University, Tbilisi, Georgia." } @@ -25650,6 +26063,9 @@ }, { "affiliation": [ + { + "affPubRaw": "The University of Iowa, Iowa City, IA, USA" + }, { "affPubRaw": "Also at Sinop University, Sinop, Turkey." } @@ -25703,6 +26119,9 @@ }, { "affiliation": [ + { + "affPubRaw": "The University of Iowa, Iowa City, IA, USA" + }, { "affPubRaw": "Also at Erciyes University, Kayseri, Turkey." } @@ -26106,6 +26525,9 @@ }, { "affiliation": [ + { + "affPubRaw": "The University of Kansas, Lawrence, KS, USA" + }, { "affPubRaw": "Also at Horia Hulubei National Institute of Physics and Nuclear Engineering (IFIN-HH), Bucharest, Romania." } @@ -27602,6 +28024,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Northeastern University, Boston, MA, USA" + }, { "affPubRaw": "Also at Sun Yat-Sen University, Guangzhou, China." } @@ -28171,6 +28596,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "University of Notre Dame, Notre Dame, IN, USA" + } + ], "attrib": { "orcid": "0009-0006-3545-1938" }, @@ -29376,6 +29806,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "University of Rochester, Rochester, NY, USA" + } + ], "attrib": { "orcid": "0000-0001-6743-3781" }, @@ -29385,6 +29820,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "University of Rochester, Rochester, NY, USA" + } + ], "attrib": { "orcid": "0000-0001-7556-8969" }, @@ -29531,6 +29971,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Rutgers, The State University of New Jersey, Piscataway, NJ, USA" + } + ], "attrib": { "orcid": "0000-0002-2785-3762" }, @@ -29890,6 +30335,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Texas A&M University, College Station, TX, USA" + }, { "affPubRaw": "Also at Texas A&M University at Qatar, Doha, Qatar." } @@ -29960,6 +30408,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Texas A&M University, College Station, TX, USA" + }, { "affPubRaw": "Also at Kyungpook National University, Daegu, Korea." } @@ -30952,6 +31403,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + }, { "affPubRaw": "Also at another institute or international laboratory covered by a cooperation agreement with CERN." } @@ -31030,6 +31484,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + }, { "affPubRaw": "Also at another institute or international laboratory covered by a cooperation agreement with CERN." } @@ -31044,6 +31501,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + }, { "affPubRaw": "Also at another institute or international laboratory covered by a cooperation agreement with CERN." } @@ -31072,6 +31532,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + }, { "affPubRaw": "Also at another institute or international laboratory covered by a cooperation agreement with CERN." } @@ -31086,6 +31549,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + }, { "affPubRaw": "Also at Universiteit Antwerpen, Antwerpen, Belgium." } @@ -31099,6 +31565,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + } + ], "attrib": { "orcid": "0000-0002-7766-7175" }, @@ -31305,6 +31776,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + }, { "affPubRaw": "Also at another institute or international laboratory covered by a cooperation agreement with CERN." } @@ -31386,6 +31860,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + }, { "affPubRaw": "Also at another institute or international laboratory covered by a cooperation agreement with CERN." } @@ -31428,6 +31905,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + }, { "affPubRaw": "Also at Northeastern University, Boston, Massachusetts, USA." } @@ -31484,6 +31964,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + }, { "affPubRaw": "Also at another institute or international laboratory covered by a cooperation agreement with CERN." } @@ -31512,6 +31995,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + }, { "affPubRaw": "Also at Imperial College, London, United Kingdom." } @@ -31593,6 +32079,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + }, { "affPubRaw": "Also at another institute or international laboratory covered by a cooperation agreement with CERN." } @@ -31618,6 +32107,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + }, { "affPubRaw": "Also at another institute or international laboratory covered by a cooperation agreement with CERN." } @@ -31702,6 +32194,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + }, { "affPubRaw": "Also at another institute or international laboratory covered by a cooperation agreement with CERN." } @@ -31883,6 +32378,11 @@ } }, { + "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + } + ], "name": { "given_name": "A.", "surname": "Vorobyev" @@ -31918,6 +32418,9 @@ }, { "affiliation": [ + { + "affPubRaw": "Authors affiliated with an institute or an international laboratory covered by a cooperation agreement with CERN" + }, { "affPubRaw": "Also at Institute of Nuclear Physics of the Uzbekistan Academy of Sciences, Tashkent, Uzbekistan." } diff --git a/tests/stubdata/output/els_simple_article_3.json b/tests/stubdata/output/els_simple_article_3.json index 29419a9..cdaaaba 100644 --- a/tests/stubdata/output/els_simple_article_3.json +++ b/tests/stubdata/output/els_simple_article_3.json @@ -1,6 +1,11 @@ { "authors": [ { + "affiliation": [ + { + "affPubRaw": "Cognitive Electrophysiology Lab, Department of Psychology, University of Milano-Bicocca, Piazza dell'AteneoNuovo, 1, Milan 20162, Italy" + } + ], "attrib": { "email": "mado.proverbio@unimib.it", "orcid": "0000-0002-5138-1523" diff --git a/tests/stubdata/output/els_simple_article_4.json b/tests/stubdata/output/els_simple_article_4.json index fc25e52..4308779 100644 --- a/tests/stubdata/output/els_simple_article_4.json +++ b/tests/stubdata/output/els_simple_article_4.json @@ -1,6 +1,11 @@ { "authors": [ { + "affiliation": [ + { + "affPubRaw": "Institute for Pulsed Power and Microwave Technology, Karlsruhe Institute of Technology, Germany" + } + ], "attrib": { "email": "christian.gusbeth@kit.edu", "orcid": "0000-0002-1457-5994" From a27c5a75dd85b7832efa10e0f71a70c7e81685a9 Mon Sep 17 00:00:00 2001 From: Matthew Templeton Date: Sat, 27 Apr 2024 19:24:43 -0400 Subject: [PATCH 09/10] Case of coverDisplayDate of "month1-month2 year" modified: adsingestp/parsers/elsevier.py new file: tests/stubdata/input/els_odd_cover_date.xml new file: tests/stubdata/output/els_odd_cover_date.json modified: tests/test_elsevier.py --- adsingestp/parsers/elsevier.py | 17 ++ tests/stubdata/input/els_odd_cover_date.xml | 1 + tests/stubdata/output/els_odd_cover_date.json | 197 ++++++++++++++++++ tests/test_elsevier.py | 1 + 4 files changed, 216 insertions(+) create mode 100644 tests/stubdata/input/els_odd_cover_date.xml create mode 100644 tests/stubdata/output/els_odd_cover_date.json diff --git a/adsingestp/parsers/elsevier.py b/adsingestp/parsers/elsevier.py index d9d891a..2bd966e 100644 --- a/adsingestp/parsers/elsevier.py +++ b/adsingestp/parsers/elsevier.py @@ -118,6 +118,23 @@ def _parse_pubdate(self): elif regex_yyyy.match(pubdate): year = pubdate self.base_metadata["pubdate_print"] = year + "-00-00" + else: + pubdate_parts = pubdate.split() + year = None + month = None + day = None + if len(pubdate_parts) == 2: + for pp in pubdate_parts: + if regex_yyyy.match(pp): + year = pp + elif utils.MONTH_TO_NUMBER.get(pp[0:3].lower(), None): + month = utils.MONTH_TO_NUMBER.get(pp[0:3].lower(), None) + if year: + if not month: + month = "00" + if not day: + day = "00" + self.base_metadata["pubdate_print"] = "%s-%s-%s" % (year, month, day) def _parse_edhistory(self): # key: xml tag, value: self.base_metadata key diff --git a/tests/stubdata/input/els_odd_cover_date.xml b/tests/stubdata/input/els_odd_cover_date.xml new file mode 100644 index 0000000..89fed36 --- /dev/null +++ b/tests/stubdata/input/els_odd_cover_date.xml @@ -0,0 +1 @@ +application/xmlLaboratory rotational spectroscopy of the magnesium-carbon chains MgC[formula omitted]H and MgC[formula omitted]NP. Bryan ChangalaNadav Genossar-DanJoshua H. BarabanMichael C. McCarthyRotational spectroscopyMetal-ligand moleculesAstrochemistryLaser-coolable moleculesJournal of Molecular Spectroscopy 401 (2024). doi:10.1016/j.jms.2024.111904journalJournal of Molecular Spectroscopy© 2024 Elsevier Inc. All rights reserved.Elsevier Inc.0022-2852401March-April 202410.1016/j.jms.2024.111904http://dx.doi.org/10.1016/j.jms.2024.111904doi:10.1016/j.jms.2024.1119041119042024-04-12T00:00:00.000ZJournalsS250.1YJMSP111904111904S0022-2852(24)00031-610.1016/j.jms.2024.111904Elsevier Inc.Fig. 1Laser ablation-electric discharge expansion source. A solenoid valve releases a pulse of precursor gas mixture synchronized with a laser pulse that ablates a rotating cylindrical metal target positioned outside the valve. The entrained ablation products continue through a stack of discharge electrodes and supersonically expand into the vacuum microwave cavity.Fig. 2Cavity FTMW measurements of MgC4H. The N and J quantum numbers are indicated above each panel, which is plotted with respect to the frequency offset from the center frequency shown. These transitions exhibit a larger Doppler splitting due to the co-axial cavity-expansion geometry and a smaller hyperfine splitting from the Fermi contact interaction of the H nuclear spin (I=1/2). The hyperfine doublets are labeled by the total angular momentum quantum number F (F=I+J). From top to bottom, the spectra are the result of 7min, 12min, and 70min of integration, respectively.Fig. 3Cavity FTMW measurements of MgC3N. The center frequencies and (N, J, F) quantum numbers are labeled as in Fig. 2. Each spin-rotation transition is split into three 14N nuclear hyperfine components (I=1), which are incompletely resolved (and unassigned) for transitions above 14GHz. The top and bottom spectra are the result of 130min and 230min of integration, respectively.Table 1The laboratory rest frequencies of MgC4H.N′J′F′NJFFrequency (MHz)aObs. − Calc. (kHz)22.5311.525528.28330.732.5321.528286.75831.032.5221.518286.78122.833.5422.538291.29301.533.5322.528291.3098−2.843.5432.5311049.7634−7.343.5332.5211049.7818−0.544.5533.5411054.2951−0.344.5433.5311054.30740.454.5543.5413812.7767b4.554.5443.5313812.7767b−2.955.5644.5513817.2959b3.355.5544.5413817.2959b−4.165.5654.5516575.7681b4.765.5554.5416575.7681b−0.466.5755.5616580.2859b4.366.5655.5516580.2859b−0.876.5765.5619338.7484b4.776.5665.5519338.7484b0.977.5866.5719343.2618b1.277.5766.5619343.2618b−2.587.5876.5722101.7115b−0.587.5776.5622101.7115b−3.488.5977.5822106.2289b1.088.5877.5722106.2289b−1.9aThe measurement uncertainty is 2 kHz.bHyperfine splitting is unresolved. The mean transition frequency is reported.Table 2The laboratory rest frequencies of MgC3N.N′J′F′NJFFrequency (MHz)aObs. − Calc. (kHz)32.52.521.51.58283.07042.032.53.521.52.58283.23050.833.52.522.51.58287.39631.333.53.522.52.58287.44460.633.54.522.53.58287.5473−0.843.52.532.51.511044.8171−0.443.53.532.52.511044.8722−2.043.54.532.53.511044.94660.144.53.533.52.511049.21590.244.54.533.53.511049.2402−1.844.55.533.54.511049.2966−1.554.54.543.53.513806.6394−3.754.55.543.54.513806.68733.455.54.544.53.513810.9914−4.555.55.544.54.513811.02026.855.56.544.55.513811.0485−0.1aThe measurement uncertainty is 2 kHz.Table 3The spectroscopic constants of MgC4H and MgC3N.Table 4Calculated properties of MgC4H and MgC3N.ParameterMgC4HMgC3NUHFROHFUHFROHFrMgC1/Å a2.045452.044252.064242.06273rC1C2/Å1.221891.229751.219101.22679rC2C3/Å1.379791.373451.383101.37721rC3C4/C3N/Å1.204341.211471.155861.16256rC4H/Å1.061491.06171––Be/MHzb1379.2401376.4091378.3741375.641ΔBvib/MHzb–2.445b–2.629bμe/a.u.c0.8410.8342.5182.494ρMg/a.u.d0.991980.935201.061120.99916ρC1/a.u.0.109550.126290.108480.12546ρC2/a.u.0.043030.016950.043830.01705ρC3/a.u.−0.026590.00334−0.025510.00305ρC4/N/a.u.0.02412−0.000510.02044−0.00055ρH/a.u.−0.003870.00018––〈Sˆ2〉SCFe1.1960.7501.1610.750〈Sˆ2〉CC0.8150.7500.8060.750bF/MHzf−17.2770.8036.595−0.178c/MHz6.6400.053−6.4640.553eQq/MHz––−4.305−4.170Note — The optimized geometries and electronic properties were calculated at the UHF- or ROHF-CCSD(T)/cc-pCVQZ level of theory, except where otherwise noted.aThe bond lengths with C1, C2, etc., labeling the C atoms beginning with that closest to Mg.bBe is the equilibrium rotational constant. ΔBvib=B0−Be is the zero-point vibrational correction. The ΔBvib values were calculated with VPT2 using the cc-pCVTZ basis set.cThe equilibrium electric dipole moment.dThe unpaired spin densities evaluated at sequential nuclei.e〈Sˆ2〉SCF is the SCF expectation value of Sˆ2, and 〈Sˆ2〉CC is the projected expectation value 〈0|Sˆ2exp(Tˆ)|0〉, where Tˆ is the coupled-cluster excitation operator.fbF and c are the Fermi contact and spin-dipole hyperfine coupling constants for H/14N. eQq is the electric quadrupole coupling constant for 14N.Laboratory rotational spectroscopy of the magnesium-carbon chains MgC4H and MgC3NP. BryanChangalaWriting – review & editingWriting – original draftVisualizationValidationProject administrationMethodologyInvestigationFunding acquisitionFormal analysisConceptualizationa⁎bryan.changala@cfa.harvard.eduNadavGenossar-DanWriting – review & editingValidationInvestigationFormal analysisConceptualizationbJoshua H.BarabanWriting – review & editingValidationSupervisionProject administrationFunding acquisitionFormal analysisConceptualizationbMichael C.McCarthyWriting – review & editingSupervisionProject administrationFunding acquisitionConceptualizationaaCenter for Astrophysics — Harvard & Smithsonian, Cambridge, MA, 02138, USACenter for Astrophysics — Harvard & SmithsonianCambridgeMA02138USACenter for Astrophysics — Harvard & Smithsonian, Cambridge, MA, 02138, USAbDepartment of Chemistry, Ben-Gurion University of the Negev, Beer Sheva, 8410501, IsraelDepartment of Chemistry, Ben-Gurion University of the NegevBeer Sheva8410501IsraelDepartment of Chemistry, Ben-Gurion University of the Negev, Beer Sheva, 8410501, Israel⁎Corresponding author.AbstractRecent advances in circumstellar metal chemistry and laser-coolable molecules have spurred interest in the spectroscopy and electronic properties of alkaline earth metal-bearing polyatomic molecules. We report the microwave rotational spectra of two members of this important chemical family, the linear magnesium-carbon chains MgC4H and MgC3N, detected with cavity Fourier transform microwave spectroscopy of a laser ablation-electric discharge expansion. The rotation, fine, and hyperfine parameters have been derived from the precise laboratory rest frequencies. These experimental results, combined with a theoretical quantum chemical analysis, confirm the recent identification of MgC4H and MgC3N in the circumstellar envelope of the evolved carbon-rich star IRC+10216. The spectroscopic data also provide insight into the structural and electronic properties that influence the metal-based optical cycling center in this unique class of laser-coolable polyatomics.Graphical abstractHighlights•MgC4H and MgC3N were detected in the laboratory with microwave spectroscopy.•Confirmation of the astronomical identification in carbon-rich circumstellar envelopes.•Fine and hyperfine structure reveals a highly metal-localized unpaired electron.KeywordsRotational spectroscopyMetal-ligand moleculesAstrochemistryLaser-coolable moleculesData availabilityData will be made available on request.1IntroductionRadio astronomical observations of the evolved carbon-rich star IRC+10216 have revealed a rich metal chemistry in its inner layers and circumstellar shell. Equilibrium and non-equilibrium processes are thought to produce a large number of gas-phase molecules with highly ionic metal-ligand bonds, including small cyanides, isocyanides and acetylides [1–10]. Of these, the magnesium-carbon chains and clusters are by far the most extensively characterized family of metal-bearing circumstellar molecules. The identification of Mg(CC)nH, Mg(CC)n−1 (NC/CN), and HMg(CC)n−1(NC/CN) chains up to n=3[7,8,10–14]; their positively charged ions with n= 2–3 [15]; and the cyclic MgC2 metal dicarbide [16] in IRC+10216 provides strong support for an ion–molecule radiative association–dissociative recombination pathway that incorporates metal atoms into polyatomic molecules in the circumstellar shell [17–19]. Although an extensive literature of optical laboratory data exists for many of these Mg-bearing species [20–27], high resolution microwave/mm-wave laboratory spectra are known only for the smallest members: MgCCH [28–31], MgCN/MgNC/HMgNC [7,11,32–34], and MgC2[16]. The astronomical identification of the longer-chain molecules by radio detection has therefore relied primarily on quantum chemical calculations [13–15], motivating a renewed effort to produce these species in the laboratory and measure their rotational rest frequencies to high accuracy.Alkaline earth metal-containing molecules are also of fundamental interest in molecular physics. Ionic monovalent metal-ligand compounds (ML, with L = OH, OCH3, CCH, etc.) are the most common polyatomic candidates for direct laser-cooling applications because of the unique electronic structure of the unpaired electron localized on the metal atom [35,36]. This optically active electron interacts only weakly with the rest of the molecule, giving rise to quasi-atomic metal-centered electronic excitations with highly diagonal vibrational Franck–Condon factors, which are necessary for efficient photon cycling schemes. Metal acetylides are intriguing laser-cooling candidates in this class because they can potentially accommodate multiple metal atoms whose interactions can be tuned by simply elongating the chain with repeated C≡C units, i.e., M−(CC)n−M′[37,38]. Quantifying the precise structural and electronic properties of long alkaline-earth metal-carbon chains is therefore crucial to illuminating the chemical design principles of these complex laser-coolable polyatomics [30].Motivated by these astrophysical and fundamental considerations, we have produced MgC4H and MgC3N in the laboratory with a laser ablation-electric discharge supersonic expansion source and detected their rotational spectra with a sensitive cavity Fourier transform microwave (FTMW) spectrometer. The precise spectroscopic constants derived from the laboratory rest frequencies are consistent with those derived from recent astronomical observations [13]. When combined with a variety of additional laboratory assays and tests, and new theoretical calculations, these measurements confirm beyond any reasonable doubt the identification of MgC4H and MgC3N in IRC+10216. A comparison of the structural and electronic properties inferred from their rotational, fine, and hyperfine parameters with those of the shorter analogues (e.g., MgCCH and MgCN) provides insight into the chemical and electronic trends of this important family of metal-ligand molecules.2ExperimentalMgC4H and MgC3N were produced in a laser ablation-electric discharge expansion source at conditions similar to those of other closely-related alkaline earth metal-bearing molecules recently studied in our laboratory, including MgCCH [30] and MgC2[16] (see Fig. 1). A dilute mixture of organic precursors in neon (∼0.1% acetylene, diacetylene, or acetonitrile) was expanded into a large vacuum chamber through a pulsed solenoid valve operating at a 5 Hz repetition rate with a ∼500μs pulse length. After the gas exits the valve, it passes a rotating magnesium rod that was ablated by a 5ns, 20–40 mJ pulse of 532 nm radiation generated from an Nd:YAG laser. The timing is such that the ablation plume is entrained into the expanding gas and then passes through two cylindrical copper electrodes separated by 1 cm and biased with a 700–900 V potential, which drives a 20–40 mA discharge current. The discharge increased the MgC4H and MgC3N yields by up to a factor of 5 relative to ablation alone likely due to the enhanced reactivity of electronically excited Mg∗ atoms or Mg+ cations [30,31,39,40].The rotational spectra were measured with a cavity FTMW spectrometer operating from 5 to 26 GHz [41,42]. The cavity is aligned co-axially with the supersonic expansion and surrounded by three pairs of Helmholtz coils tuned to cancel the Earth’s magnetic field, which causes Zeeman splitting and shifts of the rotational transitions of open-shell molecules. Residual magnetic fields near the cavity boundaries are estimated to be less than 50 mG, and the rest frequencies of the rotational transitions were measured to an accuracy of 2 kHz.Using the spectroscopic parameters of putative MgC4H and MgC3N derived from astronomical observations (which span 30–110 GHz [13]), rest frequencies of both molecules in the 5–26 GHz bandwidth of the cavity spectrometer were predicted to an accuracy of 100kHz, sufficiently small to be searched for at a single position of the microwave cavity, which has very high sensitivity but a narrow instantaneous bandwidth, i.e. <0.5MHz. Microwave features of both MgC4H and MgC3N were readily observed after optimizing the experimental conditions for the production of MgCCH. Various assays were then performed to better constrain the chemical composition and properties of these carriers. Both required the ablation laser to be on, indicating they contain magnesium. The MgC4H transitions were observed with both acetylene and diacetylene precursors, but with a larger signal intensity (up to a factor of 2) from the latter. The optimal concentration of either precursor was 0.15% in neon. The MgC3N transitions required the presence of acetonitrile as a nitrogen source. A 1:1 acetonitrile:acetylene mixture (both 0.08% in neon) optimized the MgC3N signal, which was slightly more intense than that without acetylene (i.e. a pure 0.08% acetonitrile precursor). Both MgC4H and MgC3N transitions were sensitive to applied magnetic fields, displaying characteristic Zeeman splittings when one of the Helmholtz coils was turned off, as expected for an open-shell molecule. By examining the dependence of the signal on the microwave excitation power, we estimated that MgC4H has a dipole moment comparable to MgCCH (calculated to be 2.3 D and 1.7 D, respectively [43,44]) and that MgC3N has a dipole moment comparable to MgNC (calculated and measured to be 6.4 D and 5.3 D, respectively [13,26]). Accounting for the dipole moments and molecular partition functions at the typical rotational temperature of 2 K in the expansion, we estimate MgC4H and MgC3N to be a factor of 10–100 less abundant than MgCCH and MgNC, respectively, at the ablation-discharge expansion conditions optimized for MgC4H/MgC3N production, as described above. It is worth noting that a prior attempt to produce MgC3N (and CaC3N) in another laboratory equipped with a similar laser ablation expansion source, but using BrC3N, IC3N, or HC3N precursors, resulted in no detectable rotational transitions [45]. As the authors of that study pointed out, a possible explanation in this instance is the formation of divalent M(C3N)2 molecules instead, following thermochemical arguments. Given our own observations of MgCCH, MgNC, and MgC4H from HCCH, CH3CN, and HC4H precursors, respectively, we would expect MgC3N to be detectable in our source with an HC3N precursor, even with laser ablation alone (i.e. no discharge). Thus, it may also be the case that, despite comparable laser ablation pulse energies, the use of a picosecond pulse in the prior experiments (compared to the nanosecond pulses used here) might influence the population of Mg∗/Mg+ atoms, which appear to be important to the formation of monovalent alkaline earth metal-ligand molecules [40], or otherwise affect the precursor chemistry.3Theoretical methodsThe structural and electronic properties of MgC4H and MgC3N were computed with coupled-cluster quantum chemical methods in Cfour[46,47]. The optimized geometries and first-order properties were calculated with analytic derivative techniques for coupled-cluster theory with single, double, and perturbative triple excitations [CCSD(T)] with both unrestricted (UHF) [48–50] and restricted open-shell (ROHF) [51,52] reference wavefunctions and correlation- consistent polarized core-valence basis sets with double, triple, and quadruple ζ functions (cc-pCVXZ, X = D, T, Q) [53–55]. All electrons except those occupying the inner-core Mg 1s orbital were correlated. As discussed further below, the quadratically convergent self-consistent field (QCSCF) code in Cfour[56] was used to address inconsistent convergence of UHF solutions using a standard DIIS algorithm [57]. Vibrational zero-point corrections to the ground-state rotational constants were derived with second-order vibrational perturbation theory (VPT2) [58] using cubic force fields calculated by finite differences.4ResultsThe laboratory rest frequencies of MgC4H and MgC3N are listed in Tables 1 and 2. Some examples of the measured line profiles for MgC4H are shown in Fig. 2. An effective Hamiltonian for a 2Σ electronic state including rotational (B), centrifugal distortion (D), spin-rotation (γ), Fermi contact (bF), spin-dipole (c, MgC3N only), and electric quadrupole coupling (eQq, MgC3N only) parameters was fit to the measured lines using the SPFIT/SPCAT programs [59]. The small hyperfine parameters in MgC4H produced observable splittings only for transitions with N≤3, and its spectrum could be fit to the measurement uncertainty with a Fermi contact term only, fixing c=0. MgC3N exhibits much larger hyperfine splittings at low N owing to the electric quadrupole moment of the 14N nucleus (I=1). The partial collapse of the quadrupole splitting at high N led to congestion of MgC3N transitions above 14 GHz, which were excluded from the laboratory analysis because the hyperfine-weighted line center could not be confidently determined (see Fig. 3). The spectroscopic parameters derived from a laboratory-only data set and a combined laboratory-astronomical data set incorporating the 30–110 GHz transitions reported in Ref. [13] are summarized in Table 3. Although the astronomical frequencies have much larger measurement uncertainties (0.1–1.0 MHz) than the laboratory frequencies (2 kHz), the higher frequency range of the former helps to reduce the uncertainties of the derived B and D parameters. The rest frequencies calculated with the combined fit parameters for the strongest transitions below 40 GHz have a predicted uncertainty of ∼1–10 kHz. The raw line lists and fitting files are available in a permanent online data repository [60].The optimized geometry and first-order electronic properties of MgC4H and MgC3N at the CCSD(T)/cc-pCVQZ level of theory are summarized in Table 4, which includes results for both UHF and ROHF reference wavefunctions. The 〈Sˆ2〉 expectation value of the UHF reference wavefunction is ∼1.2 for both MgC4H and MgC3N, which is evidence of significant spin contamination that is only partly removed in the correlated wavefunction. (The exact value for a doublet state is 3/4.) The UHF and ROHF optimized bond lengths show differences of up to ∼0.008 Å, while the difference in quantities that depend on the unpaired spin density are even more pronounced. For example, the UHF and ROHF predictions for the magnetic hyperfine coupling constants (bF and c) for both H and 14N differ substantially in absolute magnitude and sign. Molecular properties that depend on the total electron density such as the electric dipole moment and electric quadrupole coupling constant of 14N exhibit much smaller UHF-ROHF differences.In the course of this work, it was observed that two different UHF solutions could be converged depending on the choice of SCF algorithm (DIIS or QCSCF) and basis set. The results in Table 4 correspond to the spin-contaminated solution, which was always found by the QCSCF solver and appears to be the rigorous variational minimum. For MgC3N with the cc-pCV(D,T,Q)Z basis sets and MgC4H with the cc-pCV(D,T)Z basis sets, a conventional DIIS algorithm converged a weakly spin-contaminated solution (〈Sˆ2〉CC−3/4<10−3). This weakly contaminated UHF reference wavefunction yielded optimized CCSD(T) bond lengths that differed from the ROHF-CCSD(T) values by 10−4 Å or less. Nonetheless, despite the similar optimized structures, the unpaired spin density of the weakly contaminated UHF-CCSD(T) wavefunction still differed substantially from that of the ROHF-CCSD(T) wavefunction. The values of the bF and c parameters of MgC3N with the former, for example, were 1.426 MHz and 2.157 MHz, respectively, which are considerably larger than the ROHF predictions in Table 4. (The weakly spin contaminated UHF solution could not be found for MgC4H with the cc-pCVQZ basis set.)5DiscussionThe combined laboratory, theoretical, and astronomical evidence unambiguously confirms the identification of MgC4H and MgC3N in IRC+10216 by Cernicharo et al. [13]. The next longer chains, MgC6H and MgC5N, have also been detected by radio astronomy in this source [14]. If the MgCCH:MgC4H ≈101:1–102:1 abundance ratio in our laser ablation-electric discharge holds for MgC4H:MgC6H (and similarly for MgC5N), then it should be possible to detect both of the longer species at similar experimental conditions, particularly as the laboratory rest frequencies in the cm-wave band can be predicted with relatively small uncertainties (≪1 MHz) using the astronomically derived spectroscopic constants.The structural and electronic properties of MgC4H and MgC3N demonstrate that their ionic metal-carbon bonding is very similar to that of their smaller chain analogues. Although the lack of isotopic data prevents a complete structural analysis at this juncture, if we constrain all bond lengths other than the Mg–C bond to their optimized ROHF-CCSD(T)/cc-pCVQZ values, then the semi-experimental equilibrium rotational constants, Bse=B0−ΔBvib, derived from the measured B0 values and theoretical vibrational corrections (Table 4) imply that the semi-experimental equilibrium metal-carbon bond lengths are rse(Mg–C4H) ≈2.039Å and rse(Mg–C3N) ≈2.057Å. These are similar to the Mg–C bond length in MgCCH (rse= 2.0369(7)Å [30]) and somewhat shorter than that in MgCN (∼2.072Å [32,61]). In the (usually very good) approximation that the spin-rotation constants (γ) are dominated by second-order spin–orbit contributions [62], the ratio γ/B can also be compared between different Mg-bearing chain molecules to assess changes between the electronic state manifold of the unpaired σ(sp) electron centered on the Mg atom. The γ/B values of MgC4H and MgC3N are 3.27×10−3 and 3.17×10−3, respectively, while the values for MgCCH and MgCN are 3.36×10−3[29–31] and 2.95×10−3[32]. The small spread (∼10%) of these ratios illustrates that the unpaired Mg-centered electron in each of these molecules experiences a similar electronic environment.The strong localization of the unpaired electron is also reflected by the small magnitude of the magnetic hyperfine parameters of the H and N nuclei, which are farthest from the Mg radical center. The good agreement between the calculated ROHF-CCSD(T) hyperfine parameters and the measured bF(H), bF(N), and c(N) values highlights the importance of beginning with a ROHF determinant and the high sensitivity of these properties to even small amounts of spin contamination. The unpaired spin densities at each nucleus, reported in Table 4, decay approximately exponentially with distance from the Mg atom, a pattern similar to that observed experimentally in isotopologues of MgCCH, CaCCH, and SrCCH [30]. This behavior bolsters the idea that biradical electronic interactions in M–(C≡C)n–M′ chains can potentially be tuned over several orders of magnitude by varying the number of C2 linker units. Controlling this coupling will have an important influence on the optical cycling properties of hypermetallic polyatomic molecules for next-generation laser-cooling applications [37,38].6ConclusionsThe linear magnesium-carbon chains MgC4H and MgC3N were detected and characterized at high-resolution in the laboratory by cavity FTMW spectroscopy. A parallel quantum chemical analysis highlighted the influence of spin contamination on accurate predictions of their structural and magnetic hyperfine parameters. This study lays the foundation for a number of follow-up investigations targeting their substituted isotopic species, positively and negatively charged ions, and hypermetallic derivatives. The characterization of these molecules will provide the spectroscopic data needed to critically assess the chemical evolution of metal-carbon chains in astrophysical environments and the suitability of their unique electronic structure for applications in fundamental molecular physics.CRediT authorship contribution statementP. Bryan Changala: Writing – review & editing, Writing – original draft, Visualization, Validation, Project administration, Methodology, Investigation, Funding acquisition, Formal analysis, Conceptualization. Nadav Genossar-Dan: Writing – review & editing, Validation, Investigation, Formal analysis, Conceptualization. Joshua H. Baraban: Writing – review & editing, Validation, Supervision, Project administration, Funding acquisition, Formal analysis, Conceptualization. Michael C. McCarthy: Writing – review & editing, Supervision, Project administration, Funding acquisition, Conceptualization.Declaration of competing interestThe authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.AcknowledgmentsThe authors thank Prof. John F. Stanton (University of Florida) for helpful discussions regarding spin contamination. This work was supported by the U.S. National Science Foundation Award Nos. PHY-2110489 and AST-1908576, and by the U.S.-Israel Binational Science Foundation (Grant No. 2020724). N.G.-D. and J.H.B. are also supported by the Israel Science Foundation (ISF) , Grant No. 194/20. N.G.-D. acknowledges the VATAT scholarship for Ph.D. students in quantum science and technology.References[1]TurnerB.E.SteimleT.C.MeertsL.Detection of sodium cyanide (NaCN) in IRC 10216Astrophys. J. 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A 271 (1963) 424–434. doi:10.1098/rspa.1963.0027. https://royalsocietypublishing.org/doi/10.1098/rspa.1963.0027 \ No newline at end of file diff --git a/tests/stubdata/output/els_odd_cover_date.json b/tests/stubdata/output/els_odd_cover_date.json new file mode 100644 index 0000000..4399529 --- /dev/null +++ b/tests/stubdata/output/els_odd_cover_date.json @@ -0,0 +1,197 @@ +{ + "abstract": { + "textEnglish": "Recent advances in circumstellar metal chemistry and laser-coolable molecules have spurred interest in the spectroscopy and electronic properties of alkaline earth metal-bearing polyatomic molecules. We report the microwave rotational spectra of two members of this important chemical family, the linear magnesium-carbon chains MgC4H and MgC3N, detected with cavity Fourier transform microwave spectroscopy of a laser ablation-electric discharge expansion. The rotation, fine, and hyperfine parameters have been derived from the precise laboratory rest frequencies. These experimental results, combined with a theoretical quantum chemical analysis, confirm the recent identification of MgC4H and MgC3N in the circumstellar envelope of the evolved carbon-rich star IRC+10216. The spectroscopic data also provide insight into the structural and electronic properties that influence the metal-based optical cycling center in this unique class of laser-coolable polyatomics." + }, + "authors": [ + { + "affiliation": [ + { + "affPubRaw": "Center for Astrophysics \u2014 Harvard & Smithsonian, Cambridge, MA, 02138, USA" + } + ], + "attrib": { + "email": "bryan.changala@cfa.harvard.edu", + "orcid": "0000-0003-0304-9814" + }, + "name": { + "given_name": "P. Bryan", + "surname": "Changala" + } + }, + { + "affiliation": [ + { + "affPubRaw": "Department of Chemistry, Ben-Gurion University of the Negev, Beer Sheva, 8410501, Israel" + } + ], + "name": { + "given_name": "Nadav", + "surname": "Genossar-Dan" + } + }, + { + "affiliation": [ + { + "affPubRaw": "Department of Chemistry, Ben-Gurion University of the Negev, Beer Sheva, 8410501, Israel" + } + ], + "name": { + "given_name": "Joshua H.", + "surname": "Baraban" + } + }, + { + "affiliation": [ + { + "affPubRaw": "Center for Astrophysics \u2014 Harvard & Smithsonian, Cambridge, MA, 02138, USA" + } + ], + "name": { + "given_name": "Michael C.", + "surname": "McCarthy" + } + } + ], + "copyright": { + "statement": "\u00a9 2024 Elsevier Inc. All rights reserved.", + "status": true + }, + "doctype": "article", + "editorialHistory": { + "acceptedDate": "2024-04-09", + "receivedDates": [ + "2024-01-22" + ], + "revisedDates": [ + "2024-04-07" + ] + }, + "esources": [ + { + "location": "http://dx.doi.org/10.1016/j.jms.2024.111904", + "source": "pub_html" + } + ], + "keywords": [ + { + "keyString": "Rotational spectroscopy", + "keySystem": "Elsevier" + }, + { + "keyString": "Metal-ligand molecules", + "keySystem": "Elsevier" + }, + { + "keyString": "Astrochemistry", + "keySystem": "Elsevier" + }, + { + "keyString": "Laser-coolable molecules", + "keySystem": "Elsevier" + } + ], + "pagination": { + "electronicID": "111904" + }, + "persistentIDs": [ + { + "DOI": "10.1016/j.jms.2024.111904" + } + ], + "pubDate": { + "printDate": "2024-03-00" + }, + "publication": { + "ISSN": [ + { + "issnString": "0022-2852", + "pubtype": "not specified" + } + ], + "pubName": "Journal of Molecular Spectroscopy", + "pubYear": "2024", + "publisher": "Elsevier Inc.", + "volumeNum": "401" + }, + "publisherIDs": [ + { + "Identifier": "S0022-2852(24)00031-6", + "attribute": "PII" + } + ], + "recordData": { + "createdTime": "", + "loadFormat": "OtherXML", + "loadLocation": "", + "loadType": "fromFile", + "parsedTime": "", + "recordOrigin": "" + }, + "references": [ + "TurnerB.E.SteimleT.C.MeertsL.Detection of sodium cyanide (NaCN) in IRC 10216Astrophys. 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Phys.11921\u201322202110.1080/00268976.2021.1974590URL https://www.tandfonline.com/doi/full/10.1080/00268976.2021.1974590", + "PulayP.Improved SCF convergence accelerationJ. Comput. Chem.3198255656010.1002/jcc.540030413URL https://onlinelibrary.wiley.com/doi/10.1002/jcc.540030413", + "MillsI.M.Vibration-rotation structure in asymmetric- and symmetric-top moleculesRaoK.N.MathewsC.W.Molecular Spectroscopy: Modern Research1972Academic PressNew York115140Ch. 3.2", + "PickettH.M.The fitting and prediction of vibration-rotation spectra with spin interactionsJ. Mol. Spectrosc.148199137137710.1016/0022-2852(91)90393-O", + "ChangalaP.B.Genossar-DanN.BarabanJ.H.McCarthyM.C.Data for \u201claboratory rotational spectroscopy of the magnesium-carbon chains MgC4H and MgC3N\u201d202410.5281/zenodo.10779111", + "HiranoT.IshiiK.OdakaT.E.JensenP.A theoretical study of MgNC and MgCN in the X\u03032\u03a3+ electronic stateJ. Mol. Spectrosc.2152002425710.1006/jmsp.2002.8598URL https://linkinghub.elsevier.com/retrieve/pii/S002228520298598X", + "StoneA.J.Gauge invariance of the g tensorProc. Roy. Soc. A271196342443410.1098/rspa.1963.0027URL https://royalsocietypublishing.org/doi/10.1098/rspa.1963.0027" + ], + "title": { + "textEnglish": "Laboratory rotational spectroscopy of the magnesium-carbon chains MgC4H and MgC3N" + } +} diff --git a/tests/test_elsevier.py b/tests/test_elsevier.py index 260dabb..7481b7c 100644 --- a/tests/test_elsevier.py +++ b/tests/test_elsevier.py @@ -35,6 +35,7 @@ def test_elsevier(self): "els_detag_example_2", "els_list", "els_phlb_compound_affil", + "els_odd_cover_date", ] for f in filenames: test_infile = os.path.join(self.inputdir, f + ".xml") From 06d2394abf814c1f85159babfde1ed13f7cd0eb1 Mon Sep 17 00:00:00 2001 From: Matthew Templeton Date: Sat, 27 Apr 2024 19:27:47 -0400 Subject: [PATCH 10/10] Fix linter issue modified: tests/stubdata/input/els_odd_cover_date.xml --- tests/stubdata/input/els_odd_cover_date.xml | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/tests/stubdata/input/els_odd_cover_date.xml b/tests/stubdata/input/els_odd_cover_date.xml index 89fed36..423d6bb 100644 --- a/tests/stubdata/input/els_odd_cover_date.xml +++ b/tests/stubdata/input/els_odd_cover_date.xml @@ -1 +1 @@ -application/xmlLaboratory rotational spectroscopy of the magnesium-carbon chains MgC[formula omitted]H and MgC[formula omitted]NP. Bryan ChangalaNadav Genossar-DanJoshua H. BarabanMichael C. McCarthyRotational spectroscopyMetal-ligand moleculesAstrochemistryLaser-coolable moleculesJournal of Molecular Spectroscopy 401 (2024). doi:10.1016/j.jms.2024.111904journalJournal of Molecular Spectroscopy© 2024 Elsevier Inc. All rights reserved.Elsevier Inc.0022-2852401March-April 202410.1016/j.jms.2024.111904http://dx.doi.org/10.1016/j.jms.2024.111904doi:10.1016/j.jms.2024.1119041119042024-04-12T00:00:00.000ZJournalsS250.1YJMSP111904111904S0022-2852(24)00031-610.1016/j.jms.2024.111904Elsevier Inc.Fig. 1Laser ablation-electric discharge expansion source. A solenoid valve releases a pulse of precursor gas mixture synchronized with a laser pulse that ablates a rotating cylindrical metal target positioned outside the valve. The entrained ablation products continue through a stack of discharge electrodes and supersonically expand into the vacuum microwave cavity.Fig. 2Cavity FTMW measurements of MgC4H. The N and J quantum numbers are indicated above each panel, which is plotted with respect to the frequency offset from the center frequency shown. These transitions exhibit a larger Doppler splitting due to the co-axial cavity-expansion geometry and a smaller hyperfine splitting from the Fermi contact interaction of the H nuclear spin (I=1/2). The hyperfine doublets are labeled by the total angular momentum quantum number F (F=I+J). From top to bottom, the spectra are the result of 7min, 12min, and 70min of integration, respectively.Fig. 3Cavity FTMW measurements of MgC3N. The center frequencies and (N, J, F) quantum numbers are labeled as in Fig. 2. Each spin-rotation transition is split into three 14N nuclear hyperfine components (I=1), which are incompletely resolved (and unassigned) for transitions above 14GHz. The top and bottom spectra are the result of 130min and 230min of integration, respectively.Table 1The laboratory rest frequencies of MgC4H.N′J′F′NJFFrequency (MHz)aObs. − Calc. (kHz)22.5311.525528.28330.732.5321.528286.75831.032.5221.518286.78122.833.5422.538291.29301.533.5322.528291.3098−2.843.5432.5311049.7634−7.343.5332.5211049.7818−0.544.5533.5411054.2951−0.344.5433.5311054.30740.454.5543.5413812.7767b4.554.5443.5313812.7767b−2.955.5644.5513817.2959b3.355.5544.5413817.2959b−4.165.5654.5516575.7681b4.765.5554.5416575.7681b−0.466.5755.5616580.2859b4.366.5655.5516580.2859b−0.876.5765.5619338.7484b4.776.5665.5519338.7484b0.977.5866.5719343.2618b1.277.5766.5619343.2618b−2.587.5876.5722101.7115b−0.587.5776.5622101.7115b−3.488.5977.5822106.2289b1.088.5877.5722106.2289b−1.9aThe measurement uncertainty is 2 kHz.bHyperfine splitting is unresolved. The mean transition frequency is reported.Table 2The laboratory rest frequencies of MgC3N.N′J′F′NJFFrequency (MHz)aObs. − Calc. (kHz)32.52.521.51.58283.07042.032.53.521.52.58283.23050.833.52.522.51.58287.39631.333.53.522.52.58287.44460.633.54.522.53.58287.5473−0.843.52.532.51.511044.8171−0.443.53.532.52.511044.8722−2.043.54.532.53.511044.94660.144.53.533.52.511049.21590.244.54.533.53.511049.2402−1.844.55.533.54.511049.2966−1.554.54.543.53.513806.6394−3.754.55.543.54.513806.68733.455.54.544.53.513810.9914−4.555.55.544.54.513811.02026.855.56.544.55.513811.0485−0.1aThe measurement uncertainty is 2 kHz.Table 3The spectroscopic constants of MgC4H and MgC3N.Table 4Calculated properties of MgC4H and MgC3N.ParameterMgC4HMgC3NUHFROHFUHFROHFrMgC1/Å a2.045452.044252.064242.06273rC1C2/Å1.221891.229751.219101.22679rC2C3/Å1.379791.373451.383101.37721rC3C4/C3N/Å1.204341.211471.155861.16256rC4H/Å1.061491.06171––Be/MHzb1379.2401376.4091378.3741375.641ΔBvib/MHzb–2.445b–2.629bμe/a.u.c0.8410.8342.5182.494ρMg/a.u.d0.991980.935201.061120.99916ρC1/a.u.0.109550.126290.108480.12546ρC2/a.u.0.043030.016950.043830.01705ρC3/a.u.−0.026590.00334−0.025510.00305ρC4/N/a.u.0.02412−0.000510.02044−0.00055ρH/a.u.−0.003870.00018––〈Sˆ2〉SCFe1.1960.7501.1610.750〈Sˆ2〉CC0.8150.7500.8060.750bF/MHzf−17.2770.8036.595−0.178c/MHz6.6400.053−6.4640.553eQq/MHz––−4.305−4.170Note — The optimized geometries and electronic properties were calculated at the UHF- or ROHF-CCSD(T)/cc-pCVQZ level of theory, except where otherwise noted.aThe bond lengths with C1, C2, etc., labeling the C atoms beginning with that closest to Mg.bBe is the equilibrium rotational constant. ΔBvib=B0−Be is the zero-point vibrational correction. The ΔBvib values were calculated with VPT2 using the cc-pCVTZ basis set.cThe equilibrium electric dipole moment.dThe unpaired spin densities evaluated at sequential nuclei.e〈Sˆ2〉SCF is the SCF expectation value of Sˆ2, and 〈Sˆ2〉CC is the projected expectation value 〈0|Sˆ2exp(Tˆ)|0〉, where Tˆ is the coupled-cluster excitation operator.fbF and c are the Fermi contact and spin-dipole hyperfine coupling constants for H/14N. eQq is the electric quadrupole coupling constant for 14N.Laboratory rotational spectroscopy of the magnesium-carbon chains MgC4H and MgC3NP. BryanChangalaWriting – review & editingWriting – original draftVisualizationValidationProject administrationMethodologyInvestigationFunding acquisitionFormal analysisConceptualizationa⁎bryan.changala@cfa.harvard.eduNadavGenossar-DanWriting – review & editingValidationInvestigationFormal analysisConceptualizationbJoshua H.BarabanWriting – review & editingValidationSupervisionProject administrationFunding acquisitionFormal analysisConceptualizationbMichael C.McCarthyWriting – review & editingSupervisionProject administrationFunding acquisitionConceptualizationaaCenter for Astrophysics — Harvard & Smithsonian, Cambridge, MA, 02138, USACenter for Astrophysics — Harvard & SmithsonianCambridgeMA02138USACenter for Astrophysics — Harvard & Smithsonian, Cambridge, MA, 02138, USAbDepartment of Chemistry, Ben-Gurion University of the Negev, Beer Sheva, 8410501, IsraelDepartment of Chemistry, Ben-Gurion University of the NegevBeer Sheva8410501IsraelDepartment of Chemistry, Ben-Gurion University of the Negev, Beer Sheva, 8410501, Israel⁎Corresponding author.AbstractRecent advances in circumstellar metal chemistry and laser-coolable molecules have spurred interest in the spectroscopy and electronic properties of alkaline earth metal-bearing polyatomic molecules. We report the microwave rotational spectra of two members of this important chemical family, the linear magnesium-carbon chains MgC4H and MgC3N, detected with cavity Fourier transform microwave spectroscopy of a laser ablation-electric discharge expansion. The rotation, fine, and hyperfine parameters have been derived from the precise laboratory rest frequencies. These experimental results, combined with a theoretical quantum chemical analysis, confirm the recent identification of MgC4H and MgC3N in the circumstellar envelope of the evolved carbon-rich star IRC+10216. The spectroscopic data also provide insight into the structural and electronic properties that influence the metal-based optical cycling center in this unique class of laser-coolable polyatomics.Graphical abstractHighlights•MgC4H and MgC3N were detected in the laboratory with microwave spectroscopy.•Confirmation of the astronomical identification in carbon-rich circumstellar envelopes.•Fine and hyperfine structure reveals a highly metal-localized unpaired electron.KeywordsRotational spectroscopyMetal-ligand moleculesAstrochemistryLaser-coolable moleculesData availabilityData will be made available on request.1IntroductionRadio astronomical observations of the evolved carbon-rich star IRC+10216 have revealed a rich metal chemistry in its inner layers and circumstellar shell. Equilibrium and non-equilibrium processes are thought to produce a large number of gas-phase molecules with highly ionic metal-ligand bonds, including small cyanides, isocyanides and acetylides [1–10]. Of these, the magnesium-carbon chains and clusters are by far the most extensively characterized family of metal-bearing circumstellar molecules. The identification of Mg(CC)nH, Mg(CC)n−1 (NC/CN), and HMg(CC)n−1(NC/CN) chains up to n=3[7,8,10–14]; their positively charged ions with n= 2–3 [15]; and the cyclic MgC2 metal dicarbide [16] in IRC+10216 provides strong support for an ion–molecule radiative association–dissociative recombination pathway that incorporates metal atoms into polyatomic molecules in the circumstellar shell [17–19]. Although an extensive literature of optical laboratory data exists for many of these Mg-bearing species [20–27], high resolution microwave/mm-wave laboratory spectra are known only for the smallest members: MgCCH [28–31], MgCN/MgNC/HMgNC [7,11,32–34], and MgC2[16]. The astronomical identification of the longer-chain molecules by radio detection has therefore relied primarily on quantum chemical calculations [13–15], motivating a renewed effort to produce these species in the laboratory and measure their rotational rest frequencies to high accuracy.Alkaline earth metal-containing molecules are also of fundamental interest in molecular physics. Ionic monovalent metal-ligand compounds (ML, with L = OH, OCH3, CCH, etc.) are the most common polyatomic candidates for direct laser-cooling applications because of the unique electronic structure of the unpaired electron localized on the metal atom [35,36]. This optically active electron interacts only weakly with the rest of the molecule, giving rise to quasi-atomic metal-centered electronic excitations with highly diagonal vibrational Franck–Condon factors, which are necessary for efficient photon cycling schemes. Metal acetylides are intriguing laser-cooling candidates in this class because they can potentially accommodate multiple metal atoms whose interactions can be tuned by simply elongating the chain with repeated C≡C units, i.e., M−(CC)n−M′[37,38]. Quantifying the precise structural and electronic properties of long alkaline-earth metal-carbon chains is therefore crucial to illuminating the chemical design principles of these complex laser-coolable polyatomics [30].Motivated by these astrophysical and fundamental considerations, we have produced MgC4H and MgC3N in the laboratory with a laser ablation-electric discharge supersonic expansion source and detected their rotational spectra with a sensitive cavity Fourier transform microwave (FTMW) spectrometer. The precise spectroscopic constants derived from the laboratory rest frequencies are consistent with those derived from recent astronomical observations [13]. When combined with a variety of additional laboratory assays and tests, and new theoretical calculations, these measurements confirm beyond any reasonable doubt the identification of MgC4H and MgC3N in IRC+10216. A comparison of the structural and electronic properties inferred from their rotational, fine, and hyperfine parameters with those of the shorter analogues (e.g., MgCCH and MgCN) provides insight into the chemical and electronic trends of this important family of metal-ligand molecules.2ExperimentalMgC4H and MgC3N were produced in a laser ablation-electric discharge expansion source at conditions similar to those of other closely-related alkaline earth metal-bearing molecules recently studied in our laboratory, including MgCCH [30] and MgC2[16] (see Fig. 1). A dilute mixture of organic precursors in neon (∼0.1% acetylene, diacetylene, or acetonitrile) was expanded into a large vacuum chamber through a pulsed solenoid valve operating at a 5 Hz repetition rate with a ∼500μs pulse length. After the gas exits the valve, it passes a rotating magnesium rod that was ablated by a 5ns, 20–40 mJ pulse of 532 nm radiation generated from an Nd:YAG laser. The timing is such that the ablation plume is entrained into the expanding gas and then passes through two cylindrical copper electrodes separated by 1 cm and biased with a 700–900 V potential, which drives a 20–40 mA discharge current. The discharge increased the MgC4H and MgC3N yields by up to a factor of 5 relative to ablation alone likely due to the enhanced reactivity of electronically excited Mg∗ atoms or Mg+ cations [30,31,39,40].The rotational spectra were measured with a cavity FTMW spectrometer operating from 5 to 26 GHz [41,42]. The cavity is aligned co-axially with the supersonic expansion and surrounded by three pairs of Helmholtz coils tuned to cancel the Earth’s magnetic field, which causes Zeeman splitting and shifts of the rotational transitions of open-shell molecules. Residual magnetic fields near the cavity boundaries are estimated to be less than 50 mG, and the rest frequencies of the rotational transitions were measured to an accuracy of 2 kHz.Using the spectroscopic parameters of putative MgC4H and MgC3N derived from astronomical observations (which span 30–110 GHz [13]), rest frequencies of both molecules in the 5–26 GHz bandwidth of the cavity spectrometer were predicted to an accuracy of 100kHz, sufficiently small to be searched for at a single position of the microwave cavity, which has very high sensitivity but a narrow instantaneous bandwidth, i.e. <0.5MHz. Microwave features of both MgC4H and MgC3N were readily observed after optimizing the experimental conditions for the production of MgCCH. Various assays were then performed to better constrain the chemical composition and properties of these carriers. Both required the ablation laser to be on, indicating they contain magnesium. The MgC4H transitions were observed with both acetylene and diacetylene precursors, but with a larger signal intensity (up to a factor of 2) from the latter. The optimal concentration of either precursor was 0.15% in neon. The MgC3N transitions required the presence of acetonitrile as a nitrogen source. A 1:1 acetonitrile:acetylene mixture (both 0.08% in neon) optimized the MgC3N signal, which was slightly more intense than that without acetylene (i.e. a pure 0.08% acetonitrile precursor). Both MgC4H and MgC3N transitions were sensitive to applied magnetic fields, displaying characteristic Zeeman splittings when one of the Helmholtz coils was turned off, as expected for an open-shell molecule. By examining the dependence of the signal on the microwave excitation power, we estimated that MgC4H has a dipole moment comparable to MgCCH (calculated to be 2.3 D and 1.7 D, respectively [43,44]) and that MgC3N has a dipole moment comparable to MgNC (calculated and measured to be 6.4 D and 5.3 D, respectively [13,26]). Accounting for the dipole moments and molecular partition functions at the typical rotational temperature of 2 K in the expansion, we estimate MgC4H and MgC3N to be a factor of 10–100 less abundant than MgCCH and MgNC, respectively, at the ablation-discharge expansion conditions optimized for MgC4H/MgC3N production, as described above. It is worth noting that a prior attempt to produce MgC3N (and CaC3N) in another laboratory equipped with a similar laser ablation expansion source, but using BrC3N, IC3N, or HC3N precursors, resulted in no detectable rotational transitions [45]. As the authors of that study pointed out, a possible explanation in this instance is the formation of divalent M(C3N)2 molecules instead, following thermochemical arguments. Given our own observations of MgCCH, MgNC, and MgC4H from HCCH, CH3CN, and HC4H precursors, respectively, we would expect MgC3N to be detectable in our source with an HC3N precursor, even with laser ablation alone (i.e. no discharge). Thus, it may also be the case that, despite comparable laser ablation pulse energies, the use of a picosecond pulse in the prior experiments (compared to the nanosecond pulses used here) might influence the population of Mg∗/Mg+ atoms, which appear to be important to the formation of monovalent alkaline earth metal-ligand molecules [40], or otherwise affect the precursor chemistry.3Theoretical methodsThe structural and electronic properties of MgC4H and MgC3N were computed with coupled-cluster quantum chemical methods in Cfour[46,47]. The optimized geometries and first-order properties were calculated with analytic derivative techniques for coupled-cluster theory with single, double, and perturbative triple excitations [CCSD(T)] with both unrestricted (UHF) [48–50] and restricted open-shell (ROHF) [51,52] reference wavefunctions and correlation- consistent polarized core-valence basis sets with double, triple, and quadruple ζ functions (cc-pCVXZ, X = D, T, Q) [53–55]. All electrons except those occupying the inner-core Mg 1s orbital were correlated. As discussed further below, the quadratically convergent self-consistent field (QCSCF) code in Cfour[56] was used to address inconsistent convergence of UHF solutions using a standard DIIS algorithm [57]. Vibrational zero-point corrections to the ground-state rotational constants were derived with second-order vibrational perturbation theory (VPT2) [58] using cubic force fields calculated by finite differences.4ResultsThe laboratory rest frequencies of MgC4H and MgC3N are listed in Tables 1 and 2. Some examples of the measured line profiles for MgC4H are shown in Fig. 2. An effective Hamiltonian for a 2Σ electronic state including rotational (B), centrifugal distortion (D), spin-rotation (γ), Fermi contact (bF), spin-dipole (c, MgC3N only), and electric quadrupole coupling (eQq, MgC3N only) parameters was fit to the measured lines using the SPFIT/SPCAT programs [59]. The small hyperfine parameters in MgC4H produced observable splittings only for transitions with N≤3, and its spectrum could be fit to the measurement uncertainty with a Fermi contact term only, fixing c=0. MgC3N exhibits much larger hyperfine splittings at low N owing to the electric quadrupole moment of the 14N nucleus (I=1). The partial collapse of the quadrupole splitting at high N led to congestion of MgC3N transitions above 14 GHz, which were excluded from the laboratory analysis because the hyperfine-weighted line center could not be confidently determined (see Fig. 3). The spectroscopic parameters derived from a laboratory-only data set and a combined laboratory-astronomical data set incorporating the 30–110 GHz transitions reported in Ref. [13] are summarized in Table 3. Although the astronomical frequencies have much larger measurement uncertainties (0.1–1.0 MHz) than the laboratory frequencies (2 kHz), the higher frequency range of the former helps to reduce the uncertainties of the derived B and D parameters. The rest frequencies calculated with the combined fit parameters for the strongest transitions below 40 GHz have a predicted uncertainty of ∼1–10 kHz. The raw line lists and fitting files are available in a permanent online data repository [60].The optimized geometry and first-order electronic properties of MgC4H and MgC3N at the CCSD(T)/cc-pCVQZ level of theory are summarized in Table 4, which includes results for both UHF and ROHF reference wavefunctions. The 〈Sˆ2〉 expectation value of the UHF reference wavefunction is ∼1.2 for both MgC4H and MgC3N, which is evidence of significant spin contamination that is only partly removed in the correlated wavefunction. (The exact value for a doublet state is 3/4.) The UHF and ROHF optimized bond lengths show differences of up to ∼0.008 Å, while the difference in quantities that depend on the unpaired spin density are even more pronounced. For example, the UHF and ROHF predictions for the magnetic hyperfine coupling constants (bF and c) for both H and 14N differ substantially in absolute magnitude and sign. Molecular properties that depend on the total electron density such as the electric dipole moment and electric quadrupole coupling constant of 14N exhibit much smaller UHF-ROHF differences.In the course of this work, it was observed that two different UHF solutions could be converged depending on the choice of SCF algorithm (DIIS or QCSCF) and basis set. The results in Table 4 correspond to the spin-contaminated solution, which was always found by the QCSCF solver and appears to be the rigorous variational minimum. For MgC3N with the cc-pCV(D,T,Q)Z basis sets and MgC4H with the cc-pCV(D,T)Z basis sets, a conventional DIIS algorithm converged a weakly spin-contaminated solution (〈Sˆ2〉CC−3/4<10−3). This weakly contaminated UHF reference wavefunction yielded optimized CCSD(T) bond lengths that differed from the ROHF-CCSD(T) values by 10−4 Å or less. Nonetheless, despite the similar optimized structures, the unpaired spin density of the weakly contaminated UHF-CCSD(T) wavefunction still differed substantially from that of the ROHF-CCSD(T) wavefunction. The values of the bF and c parameters of MgC3N with the former, for example, were 1.426 MHz and 2.157 MHz, respectively, which are considerably larger than the ROHF predictions in Table 4. (The weakly spin contaminated UHF solution could not be found for MgC4H with the cc-pCVQZ basis set.)5DiscussionThe combined laboratory, theoretical, and astronomical evidence unambiguously confirms the identification of MgC4H and MgC3N in IRC+10216 by Cernicharo et al. [13]. The next longer chains, MgC6H and MgC5N, have also been detected by radio astronomy in this source [14]. If the MgCCH:MgC4H ≈101:1–102:1 abundance ratio in our laser ablation-electric discharge holds for MgC4H:MgC6H (and similarly for MgC5N), then it should be possible to detect both of the longer species at similar experimental conditions, particularly as the laboratory rest frequencies in the cm-wave band can be predicted with relatively small uncertainties (≪1 MHz) using the astronomically derived spectroscopic constants.The structural and electronic properties of MgC4H and MgC3N demonstrate that their ionic metal-carbon bonding is very similar to that of their smaller chain analogues. Although the lack of isotopic data prevents a complete structural analysis at this juncture, if we constrain all bond lengths other than the Mg–C bond to their optimized ROHF-CCSD(T)/cc-pCVQZ values, then the semi-experimental equilibrium rotational constants, Bse=B0−ΔBvib, derived from the measured B0 values and theoretical vibrational corrections (Table 4) imply that the semi-experimental equilibrium metal-carbon bond lengths are rse(Mg–C4H) ≈2.039Å and rse(Mg–C3N) ≈2.057Å. These are similar to the Mg–C bond length in MgCCH (rse= 2.0369(7)Å [30]) and somewhat shorter than that in MgCN (∼2.072Å [32,61]). In the (usually very good) approximation that the spin-rotation constants (γ) are dominated by second-order spin–orbit contributions [62], the ratio γ/B can also be compared between different Mg-bearing chain molecules to assess changes between the electronic state manifold of the unpaired σ(sp) electron centered on the Mg atom. The γ/B values of MgC4H and MgC3N are 3.27×10−3 and 3.17×10−3, respectively, while the values for MgCCH and MgCN are 3.36×10−3[29–31] and 2.95×10−3[32]. The small spread (∼10%) of these ratios illustrates that the unpaired Mg-centered electron in each of these molecules experiences a similar electronic environment.The strong localization of the unpaired electron is also reflected by the small magnitude of the magnetic hyperfine parameters of the H and N nuclei, which are farthest from the Mg radical center. The good agreement between the calculated ROHF-CCSD(T) hyperfine parameters and the measured bF(H), bF(N), and c(N) values highlights the importance of beginning with a ROHF determinant and the high sensitivity of these properties to even small amounts of spin contamination. The unpaired spin densities at each nucleus, reported in Table 4, decay approximately exponentially with distance from the Mg atom, a pattern similar to that observed experimentally in isotopologues of MgCCH, CaCCH, and SrCCH [30]. This behavior bolsters the idea that biradical electronic interactions in M–(C≡C)n–M′ chains can potentially be tuned over several orders of magnitude by varying the number of C2 linker units. Controlling this coupling will have an important influence on the optical cycling properties of hypermetallic polyatomic molecules for next-generation laser-cooling applications [37,38].6ConclusionsThe linear magnesium-carbon chains MgC4H and MgC3N were detected and characterized at high-resolution in the laboratory by cavity FTMW spectroscopy. A parallel quantum chemical analysis highlighted the influence of spin contamination on accurate predictions of their structural and magnetic hyperfine parameters. This study lays the foundation for a number of follow-up investigations targeting their substituted isotopic species, positively and negatively charged ions, and hypermetallic derivatives. The characterization of these molecules will provide the spectroscopic data needed to critically assess the chemical evolution of metal-carbon chains in astrophysical environments and the suitability of their unique electronic structure for applications in fundamental molecular physics.CRediT authorship contribution statementP. Bryan Changala: Writing – review & editing, Writing – original draft, Visualization, Validation, Project administration, Methodology, Investigation, Funding acquisition, Formal analysis, Conceptualization. Nadav Genossar-Dan: Writing – review & editing, Validation, Investigation, Formal analysis, Conceptualization. Joshua H. Baraban: Writing – review & editing, Validation, Supervision, Project administration, Funding acquisition, Formal analysis, Conceptualization. Michael C. McCarthy: Writing – review & editing, Supervision, Project administration, Funding acquisition, Conceptualization.Declaration of competing interestThe authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.AcknowledgmentsThe authors thank Prof. John F. Stanton (University of Florida) for helpful discussions regarding spin contamination. This work was supported by the U.S. National Science Foundation Award Nos. PHY-2110489 and AST-1908576, and by the U.S.-Israel Binational Science Foundation (Grant No. 2020724). N.G.-D. and J.H.B. are also supported by the Israel Science Foundation (ISF) , Grant No. 194/20. N.G.-D. acknowledges the VATAT scholarship for Ph.D. students in quantum science and technology.References[1]TurnerB.E.SteimleT.C.MeertsL.Detection of sodium cyanide (NaCN) in IRC 10216Astrophys. J. 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Spectrosc. 215 (2002) 42–57. doi:10.1006/jmsp.2002.8598. https://linkinghub.elsevier.com/retrieve/pii/S002228520298598X[62]StoneA.J.Gauge invariance of the g tensorProc. Roy. Soc. A271196342443410.1098/rspa.1963.0027URL https://royalsocietypublishing.org/doi/10.1098/rspa.1963.0027A. J. Stone, https://royalsocietypublishing.org/doi/10.1098/rspa.1963.0027Gauge invariance of the g tensor, Proc. Roy. Soc. A 271 (1963) 424–434. doi:10.1098/rspa.1963.0027. https://royalsocietypublishing.org/doi/10.1098/rspa.1963.0027 \ No newline at end of file +application/xmlLaboratory rotational spectroscopy of the magnesium-carbon chains MgC[formula omitted]H and MgC[formula omitted]NP. Bryan ChangalaNadav Genossar-DanJoshua H. BarabanMichael C. McCarthyRotational spectroscopyMetal-ligand moleculesAstrochemistryLaser-coolable moleculesJournal of Molecular Spectroscopy 401 (2024). doi:10.1016/j.jms.2024.111904journalJournal of Molecular Spectroscopy© 2024 Elsevier Inc. All rights reserved.Elsevier Inc.0022-2852401March-April 202410.1016/j.jms.2024.111904http://dx.doi.org/10.1016/j.jms.2024.111904doi:10.1016/j.jms.2024.1119041119042024-04-12T00:00:00.000ZJournalsS250.1YJMSP111904111904S0022-2852(24)00031-610.1016/j.jms.2024.111904Elsevier Inc.Fig. 1Laser ablation-electric discharge expansion source. A solenoid valve releases a pulse of precursor gas mixture synchronized with a laser pulse that ablates a rotating cylindrical metal target positioned outside the valve. The entrained ablation products continue through a stack of discharge electrodes and supersonically expand into the vacuum microwave cavity.Fig. 2Cavity FTMW measurements of MgC4H. The N and J quantum numbers are indicated above each panel, which is plotted with respect to the frequency offset from the center frequency shown. These transitions exhibit a larger Doppler splitting due to the co-axial cavity-expansion geometry and a smaller hyperfine splitting from the Fermi contact interaction of the H nuclear spin (I=1/2). The hyperfine doublets are labeled by the total angular momentum quantum number F (F=I+J). From top to bottom, the spectra are the result of 7min, 12min, and 70min of integration, respectively.Fig. 3Cavity FTMW measurements of MgC3N. The center frequencies and (N, J, F) quantum numbers are labeled as in Fig. 2. Each spin-rotation transition is split into three 14N nuclear hyperfine components (I=1), which are incompletely resolved (and unassigned) for transitions above 14GHz. The top and bottom spectra are the result of 130min and 230min of integration, respectively.Table 1The laboratory rest frequencies of MgC4H.N′J′F′NJFFrequency (MHz)aObs. − Calc. (kHz)22.5311.525528.28330.732.5321.528286.75831.032.5221.518286.78122.833.5422.538291.29301.533.5322.528291.3098−2.843.5432.5311049.7634−7.343.5332.5211049.7818−0.544.5533.5411054.2951−0.344.5433.5311054.30740.454.5543.5413812.7767b4.554.5443.5313812.7767b−2.955.5644.5513817.2959b3.355.5544.5413817.2959b−4.165.5654.5516575.7681b4.765.5554.5416575.7681b−0.466.5755.5616580.2859b4.366.5655.5516580.2859b−0.876.5765.5619338.7484b4.776.5665.5519338.7484b0.977.5866.5719343.2618b1.277.5766.5619343.2618b−2.587.5876.5722101.7115b−0.587.5776.5622101.7115b−3.488.5977.5822106.2289b1.088.5877.5722106.2289b−1.9aThe measurement uncertainty is 2 kHz.bHyperfine splitting is unresolved. The mean transition frequency is reported.Table 2The laboratory rest frequencies of MgC3N.N′J′F′NJFFrequency (MHz)aObs. − Calc. (kHz)32.52.521.51.58283.07042.032.53.521.52.58283.23050.833.52.522.51.58287.39631.333.53.522.52.58287.44460.633.54.522.53.58287.5473−0.843.52.532.51.511044.8171−0.443.53.532.52.511044.8722−2.043.54.532.53.511044.94660.144.53.533.52.511049.21590.244.54.533.53.511049.2402−1.844.55.533.54.511049.2966−1.554.54.543.53.513806.6394−3.754.55.543.54.513806.68733.455.54.544.53.513810.9914−4.555.55.544.54.513811.02026.855.56.544.55.513811.0485−0.1aThe measurement uncertainty is 2 kHz.Table 3The spectroscopic constants of MgC4H and MgC3N.Table 4Calculated properties of MgC4H and MgC3N.ParameterMgC4HMgC3NUHFROHFUHFROHFrMgC1/Å a2.045452.044252.064242.06273rC1C2/Å1.221891.229751.219101.22679rC2C3/Å1.379791.373451.383101.37721rC3C4/C3N/Å1.204341.211471.155861.16256rC4H/Å1.061491.06171––Be/MHzb1379.2401376.4091378.3741375.641ΔBvib/MHzb–2.445b–2.629bμe/a.u.c0.8410.8342.5182.494ρMg/a.u.d0.991980.935201.061120.99916ρC1/a.u.0.109550.126290.108480.12546ρC2/a.u.0.043030.016950.043830.01705ρC3/a.u.−0.026590.00334−0.025510.00305ρC4/N/a.u.0.02412−0.000510.02044−0.00055ρH/a.u.−0.003870.00018––〈Sˆ2〉SCFe1.1960.7501.1610.750〈Sˆ2〉CC0.8150.7500.8060.750bF/MHzf−17.2770.8036.595−0.178c/MHz6.6400.053−6.4640.553eQq/MHz––−4.305−4.170Note — The optimized geometries and electronic properties were calculated at the UHF- or ROHF-CCSD(T)/cc-pCVQZ level of theory, except where otherwise noted.aThe bond lengths with C1, C2, etc., labeling the C atoms beginning with that closest to Mg.bBe is the equilibrium rotational constant. ΔBvib=B0−Be is the zero-point vibrational correction. The ΔBvib values were calculated with VPT2 using the cc-pCVTZ basis set.cThe equilibrium electric dipole moment.dThe unpaired spin densities evaluated at sequential nuclei.e〈Sˆ2〉SCF is the SCF expectation value of Sˆ2, and 〈Sˆ2〉CC is the projected expectation value 〈0|Sˆ2exp(Tˆ)|0〉, where Tˆ is the coupled-cluster excitation operator.fbF and c are the Fermi contact and spin-dipole hyperfine coupling constants for H/14N. eQq is the electric quadrupole coupling constant for 14N.Laboratory rotational spectroscopy of the magnesium-carbon chains MgC4H and MgC3NP. BryanChangalaWriting – review & editingWriting – original draftVisualizationValidationProject administrationMethodologyInvestigationFunding acquisitionFormal analysisConceptualizationa⁎bryan.changala@cfa.harvard.eduNadavGenossar-DanWriting – review & editingValidationInvestigationFormal analysisConceptualizationbJoshua H.BarabanWriting – review & editingValidationSupervisionProject administrationFunding acquisitionFormal analysisConceptualizationbMichael C.McCarthyWriting – review & editingSupervisionProject administrationFunding acquisitionConceptualizationaaCenter for Astrophysics — Harvard & Smithsonian, Cambridge, MA, 02138, USACenter for Astrophysics — Harvard & SmithsonianCambridgeMA02138USACenter for Astrophysics — Harvard & Smithsonian, Cambridge, MA, 02138, USAbDepartment of Chemistry, Ben-Gurion University of the Negev, Beer Sheva, 8410501, IsraelDepartment of Chemistry, Ben-Gurion University of the NegevBeer Sheva8410501IsraelDepartment of Chemistry, Ben-Gurion University of the Negev, Beer Sheva, 8410501, Israel⁎Corresponding author.AbstractRecent advances in circumstellar metal chemistry and laser-coolable molecules have spurred interest in the spectroscopy and electronic properties of alkaline earth metal-bearing polyatomic molecules. We report the microwave rotational spectra of two members of this important chemical family, the linear magnesium-carbon chains MgC4H and MgC3N, detected with cavity Fourier transform microwave spectroscopy of a laser ablation-electric discharge expansion. The rotation, fine, and hyperfine parameters have been derived from the precise laboratory rest frequencies. These experimental results, combined with a theoretical quantum chemical analysis, confirm the recent identification of MgC4H and MgC3N in the circumstellar envelope of the evolved carbon-rich star IRC+10216. The spectroscopic data also provide insight into the structural and electronic properties that influence the metal-based optical cycling center in this unique class of laser-coolable polyatomics.Graphical abstractHighlights•MgC4H and MgC3N were detected in the laboratory with microwave spectroscopy.•Confirmation of the astronomical identification in carbon-rich circumstellar envelopes.•Fine and hyperfine structure reveals a highly metal-localized unpaired electron.KeywordsRotational spectroscopyMetal-ligand moleculesAstrochemistryLaser-coolable moleculesData availabilityData will be made available on request.1IntroductionRadio astronomical observations of the evolved carbon-rich star IRC+10216 have revealed a rich metal chemistry in its inner layers and circumstellar shell. Equilibrium and non-equilibrium processes are thought to produce a large number of gas-phase molecules with highly ionic metal-ligand bonds, including small cyanides, isocyanides and acetylides [1–10]. Of these, the magnesium-carbon chains and clusters are by far the most extensively characterized family of metal-bearing circumstellar molecules. The identification of Mg(CC)nH, Mg(CC)n−1 (NC/CN), and HMg(CC)n−1(NC/CN) chains up to n=3[7,8,10–14]; their positively charged ions with n= 2–3 [15]; and the cyclic MgC2 metal dicarbide [16] in IRC+10216 provides strong support for an ion–molecule radiative association–dissociative recombination pathway that incorporates metal atoms into polyatomic molecules in the circumstellar shell [17–19]. Although an extensive literature of optical laboratory data exists for many of these Mg-bearing species [20–27], high resolution microwave/mm-wave laboratory spectra are known only for the smallest members: MgCCH [28–31], MgCN/MgNC/HMgNC [7,11,32–34], and MgC2[16]. The astronomical identification of the longer-chain molecules by radio detection has therefore relied primarily on quantum chemical calculations [13–15], motivating a renewed effort to produce these species in the laboratory and measure their rotational rest frequencies to high accuracy.Alkaline earth metal-containing molecules are also of fundamental interest in molecular physics. Ionic monovalent metal-ligand compounds (ML, with L = OH, OCH3, CCH, etc.) are the most common polyatomic candidates for direct laser-cooling applications because of the unique electronic structure of the unpaired electron localized on the metal atom [35,36]. This optically active electron interacts only weakly with the rest of the molecule, giving rise to quasi-atomic metal-centered electronic excitations with highly diagonal vibrational Franck–Condon factors, which are necessary for efficient photon cycling schemes. Metal acetylides are intriguing laser-cooling candidates in this class because they can potentially accommodate multiple metal atoms whose interactions can be tuned by simply elongating the chain with repeated C≡C units, i.e., M−(CC)n−M′[37,38]. Quantifying the precise structural and electronic properties of long alkaline-earth metal-carbon chains is therefore crucial to illuminating the chemical design principles of these complex laser-coolable polyatomics [30].Motivated by these astrophysical and fundamental considerations, we have produced MgC4H and MgC3N in the laboratory with a laser ablation-electric discharge supersonic expansion source and detected their rotational spectra with a sensitive cavity Fourier transform microwave (FTMW) spectrometer. The precise spectroscopic constants derived from the laboratory rest frequencies are consistent with those derived from recent astronomical observations [13]. When combined with a variety of additional laboratory assays and tests, and new theoretical calculations, these measurements confirm beyond any reasonable doubt the identification of MgC4H and MgC3N in IRC+10216. A comparison of the structural and electronic properties inferred from their rotational, fine, and hyperfine parameters with those of the shorter analogues (e.g., MgCCH and MgCN) provides insight into the chemical and electronic trends of this important family of metal-ligand molecules.2ExperimentalMgC4H and MgC3N were produced in a laser ablation-electric discharge expansion source at conditions similar to those of other closely-related alkaline earth metal-bearing molecules recently studied in our laboratory, including MgCCH [30] and MgC2[16] (see Fig. 1). A dilute mixture of organic precursors in neon (∼0.1% acetylene, diacetylene, or acetonitrile) was expanded into a large vacuum chamber through a pulsed solenoid valve operating at a 5 Hz repetition rate with a ∼500μs pulse length. After the gas exits the valve, it passes a rotating magnesium rod that was ablated by a 5ns, 20–40 mJ pulse of 532 nm radiation generated from an Nd:YAG laser. The timing is such that the ablation plume is entrained into the expanding gas and then passes through two cylindrical copper electrodes separated by 1 cm and biased with a 700–900 V potential, which drives a 20–40 mA discharge current. The discharge increased the MgC4H and MgC3N yields by up to a factor of 5 relative to ablation alone likely due to the enhanced reactivity of electronically excited Mg∗ atoms or Mg+ cations [30,31,39,40].The rotational spectra were measured with a cavity FTMW spectrometer operating from 5 to 26 GHz [41,42]. The cavity is aligned co-axially with the supersonic expansion and surrounded by three pairs of Helmholtz coils tuned to cancel the Earth’s magnetic field, which causes Zeeman splitting and shifts of the rotational transitions of open-shell molecules. Residual magnetic fields near the cavity boundaries are estimated to be less than 50 mG, and the rest frequencies of the rotational transitions were measured to an accuracy of 2 kHz.Using the spectroscopic parameters of putative MgC4H and MgC3N derived from astronomical observations (which span 30–110 GHz [13]), rest frequencies of both molecules in the 5–26 GHz bandwidth of the cavity spectrometer were predicted to an accuracy of 100kHz, sufficiently small to be searched for at a single position of the microwave cavity, which has very high sensitivity but a narrow instantaneous bandwidth, i.e. <0.5MHz. Microwave features of both MgC4H and MgC3N were readily observed after optimizing the experimental conditions for the production of MgCCH. Various assays were then performed to better constrain the chemical composition and properties of these carriers. Both required the ablation laser to be on, indicating they contain magnesium. The MgC4H transitions were observed with both acetylene and diacetylene precursors, but with a larger signal intensity (up to a factor of 2) from the latter. The optimal concentration of either precursor was 0.15% in neon. The MgC3N transitions required the presence of acetonitrile as a nitrogen source. A 1:1 acetonitrile:acetylene mixture (both 0.08% in neon) optimized the MgC3N signal, which was slightly more intense than that without acetylene (i.e. a pure 0.08% acetonitrile precursor). Both MgC4H and MgC3N transitions were sensitive to applied magnetic fields, displaying characteristic Zeeman splittings when one of the Helmholtz coils was turned off, as expected for an open-shell molecule. By examining the dependence of the signal on the microwave excitation power, we estimated that MgC4H has a dipole moment comparable to MgCCH (calculated to be 2.3 D and 1.7 D, respectively [43,44]) and that MgC3N has a dipole moment comparable to MgNC (calculated and measured to be 6.4 D and 5.3 D, respectively [13,26]). Accounting for the dipole moments and molecular partition functions at the typical rotational temperature of 2 K in the expansion, we estimate MgC4H and MgC3N to be a factor of 10–100 less abundant than MgCCH and MgNC, respectively, at the ablation-discharge expansion conditions optimized for MgC4H/MgC3N production, as described above. It is worth noting that a prior attempt to produce MgC3N (and CaC3N) in another laboratory equipped with a similar laser ablation expansion source, but using BrC3N, IC3N, or HC3N precursors, resulted in no detectable rotational transitions [45]. As the authors of that study pointed out, a possible explanation in this instance is the formation of divalent M(C3N)2 molecules instead, following thermochemical arguments. Given our own observations of MgCCH, MgNC, and MgC4H from HCCH, CH3CN, and HC4H precursors, respectively, we would expect MgC3N to be detectable in our source with an HC3N precursor, even with laser ablation alone (i.e. no discharge). Thus, it may also be the case that, despite comparable laser ablation pulse energies, the use of a picosecond pulse in the prior experiments (compared to the nanosecond pulses used here) might influence the population of Mg∗/Mg+ atoms, which appear to be important to the formation of monovalent alkaline earth metal-ligand molecules [40], or otherwise affect the precursor chemistry.3Theoretical methodsThe structural and electronic properties of MgC4H and MgC3N were computed with coupled-cluster quantum chemical methods in Cfour[46,47]. The optimized geometries and first-order properties were calculated with analytic derivative techniques for coupled-cluster theory with single, double, and perturbative triple excitations [CCSD(T)] with both unrestricted (UHF) [48–50] and restricted open-shell (ROHF) [51,52] reference wavefunctions and correlation- consistent polarized core-valence basis sets with double, triple, and quadruple ζ functions (cc-pCVXZ, X = D, T, Q) [53–55]. All electrons except those occupying the inner-core Mg 1s orbital were correlated. As discussed further below, the quadratically convergent self-consistent field (QCSCF) code in Cfour[56] was used to address inconsistent convergence of UHF solutions using a standard DIIS algorithm [57]. Vibrational zero-point corrections to the ground-state rotational constants were derived with second-order vibrational perturbation theory (VPT2) [58] using cubic force fields calculated by finite differences.4ResultsThe laboratory rest frequencies of MgC4H and MgC3N are listed in Tables 1 and 2. Some examples of the measured line profiles for MgC4H are shown in Fig. 2. An effective Hamiltonian for a 2Σ electronic state including rotational (B), centrifugal distortion (D), spin-rotation (γ), Fermi contact (bF), spin-dipole (c, MgC3N only), and electric quadrupole coupling (eQq, MgC3N only) parameters was fit to the measured lines using the SPFIT/SPCAT programs [59]. The small hyperfine parameters in MgC4H produced observable splittings only for transitions with N≤3, and its spectrum could be fit to the measurement uncertainty with a Fermi contact term only, fixing c=0. MgC3N exhibits much larger hyperfine splittings at low N owing to the electric quadrupole moment of the 14N nucleus (I=1). The partial collapse of the quadrupole splitting at high N led to congestion of MgC3N transitions above 14 GHz, which were excluded from the laboratory analysis because the hyperfine-weighted line center could not be confidently determined (see Fig. 3). The spectroscopic parameters derived from a laboratory-only data set and a combined laboratory-astronomical data set incorporating the 30–110 GHz transitions reported in Ref. [13] are summarized in Table 3. Although the astronomical frequencies have much larger measurement uncertainties (0.1–1.0 MHz) than the laboratory frequencies (2 kHz), the higher frequency range of the former helps to reduce the uncertainties of the derived B and D parameters. The rest frequencies calculated with the combined fit parameters for the strongest transitions below 40 GHz have a predicted uncertainty of ∼1–10 kHz. The raw line lists and fitting files are available in a permanent online data repository [60].The optimized geometry and first-order electronic properties of MgC4H and MgC3N at the CCSD(T)/cc-pCVQZ level of theory are summarized in Table 4, which includes results for both UHF and ROHF reference wavefunctions. The 〈Sˆ2〉 expectation value of the UHF reference wavefunction is ∼1.2 for both MgC4H and MgC3N, which is evidence of significant spin contamination that is only partly removed in the correlated wavefunction. (The exact value for a doublet state is 3/4.) The UHF and ROHF optimized bond lengths show differences of up to ∼0.008 Å, while the difference in quantities that depend on the unpaired spin density are even more pronounced. For example, the UHF and ROHF predictions for the magnetic hyperfine coupling constants (bF and c) for both H and 14N differ substantially in absolute magnitude and sign. Molecular properties that depend on the total electron density such as the electric dipole moment and electric quadrupole coupling constant of 14N exhibit much smaller UHF-ROHF differences.In the course of this work, it was observed that two different UHF solutions could be converged depending on the choice of SCF algorithm (DIIS or QCSCF) and basis set. The results in Table 4 correspond to the spin-contaminated solution, which was always found by the QCSCF solver and appears to be the rigorous variational minimum. For MgC3N with the cc-pCV(D,T,Q)Z basis sets and MgC4H with the cc-pCV(D,T)Z basis sets, a conventional DIIS algorithm converged a weakly spin-contaminated solution (〈Sˆ2〉CC−3/4<10−3). This weakly contaminated UHF reference wavefunction yielded optimized CCSD(T) bond lengths that differed from the ROHF-CCSD(T) values by 10−4 Å or less. Nonetheless, despite the similar optimized structures, the unpaired spin density of the weakly contaminated UHF-CCSD(T) wavefunction still differed substantially from that of the ROHF-CCSD(T) wavefunction. The values of the bF and c parameters of MgC3N with the former, for example, were 1.426 MHz and 2.157 MHz, respectively, which are considerably larger than the ROHF predictions in Table 4. (The weakly spin contaminated UHF solution could not be found for MgC4H with the cc-pCVQZ basis set.)5DiscussionThe combined laboratory, theoretical, and astronomical evidence unambiguously confirms the identification of MgC4H and MgC3N in IRC+10216 by Cernicharo et al. [13]. The next longer chains, MgC6H and MgC5N, have also been detected by radio astronomy in this source [14]. If the MgCCH:MgC4H ≈101:1–102:1 abundance ratio in our laser ablation-electric discharge holds for MgC4H:MgC6H (and similarly for MgC5N), then it should be possible to detect both of the longer species at similar experimental conditions, particularly as the laboratory rest frequencies in the cm-wave band can be predicted with relatively small uncertainties (≪1 MHz) using the astronomically derived spectroscopic constants.The structural and electronic properties of MgC4H and MgC3N demonstrate that their ionic metal-carbon bonding is very similar to that of their smaller chain analogues. Although the lack of isotopic data prevents a complete structural analysis at this juncture, if we constrain all bond lengths other than the Mg–C bond to their optimized ROHF-CCSD(T)/cc-pCVQZ values, then the semi-experimental equilibrium rotational constants, Bse=B0−ΔBvib, derived from the measured B0 values and theoretical vibrational corrections (Table 4) imply that the semi-experimental equilibrium metal-carbon bond lengths are rse(Mg–C4H) ≈2.039Å and rse(Mg–C3N) ≈2.057Å. These are similar to the Mg–C bond length in MgCCH (rse= 2.0369(7)Å [30]) and somewhat shorter than that in MgCN (∼2.072Å [32,61]). In the (usually very good) approximation that the spin-rotation constants (γ) are dominated by second-order spin–orbit contributions [62], the ratio γ/B can also be compared between different Mg-bearing chain molecules to assess changes between the electronic state manifold of the unpaired σ(sp) electron centered on the Mg atom. The γ/B values of MgC4H and MgC3N are 3.27×10−3 and 3.17×10−3, respectively, while the values for MgCCH and MgCN are 3.36×10−3[29–31] and 2.95×10−3[32]. The small spread (∼10%) of these ratios illustrates that the unpaired Mg-centered electron in each of these molecules experiences a similar electronic environment.The strong localization of the unpaired electron is also reflected by the small magnitude of the magnetic hyperfine parameters of the H and N nuclei, which are farthest from the Mg radical center. The good agreement between the calculated ROHF-CCSD(T) hyperfine parameters and the measured bF(H), bF(N), and c(N) values highlights the importance of beginning with a ROHF determinant and the high sensitivity of these properties to even small amounts of spin contamination. The unpaired spin densities at each nucleus, reported in Table 4, decay approximately exponentially with distance from the Mg atom, a pattern similar to that observed experimentally in isotopologues of MgCCH, CaCCH, and SrCCH [30]. This behavior bolsters the idea that biradical electronic interactions in M–(C≡C)n–M′ chains can potentially be tuned over several orders of magnitude by varying the number of C2 linker units. Controlling this coupling will have an important influence on the optical cycling properties of hypermetallic polyatomic molecules for next-generation laser-cooling applications [37,38].6ConclusionsThe linear magnesium-carbon chains MgC4H and MgC3N were detected and characterized at high-resolution in the laboratory by cavity FTMW spectroscopy. A parallel quantum chemical analysis highlighted the influence of spin contamination on accurate predictions of their structural and magnetic hyperfine parameters. This study lays the foundation for a number of follow-up investigations targeting their substituted isotopic species, positively and negatively charged ions, and hypermetallic derivatives. The characterization of these molecules will provide the spectroscopic data needed to critically assess the chemical evolution of metal-carbon chains in astrophysical environments and the suitability of their unique electronic structure for applications in fundamental molecular physics.CRediT authorship contribution statementP. Bryan Changala: Writing – review & editing, Writing – original draft, Visualization, Validation, Project administration, Methodology, Investigation, Funding acquisition, Formal analysis, Conceptualization. Nadav Genossar-Dan: Writing – review & editing, Validation, Investigation, Formal analysis, Conceptualization. Joshua H. Baraban: Writing – review & editing, Validation, Supervision, Project administration, Funding acquisition, Formal analysis, Conceptualization. Michael C. McCarthy: Writing – review & editing, Supervision, Project administration, Funding acquisition, Conceptualization.Declaration of competing interestThe authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.AcknowledgmentsThe authors thank Prof. John F. Stanton (University of Florida) for helpful discussions regarding spin contamination. This work was supported by the U.S. National Science Foundation Award Nos. PHY-2110489 and AST-1908576, and by the U.S.-Israel Binational Science Foundation (Grant No. 2020724). N.G.-D. and J.H.B. are also supported by the Israel Science Foundation (ISF) , Grant No. 194/20. N.G.-D. acknowledges the VATAT scholarship for Ph.D. students in quantum science and technology.References[1]TurnerB.E.SteimleT.C.MeertsL.Detection of sodium cyanide (NaCN) in IRC 10216Astrophys. J. 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