{"id":"W4375852878","doi":"10.1007/jhep05(2023)028","title":"Measurement of the total and differential Higgs boson production cross-sections at $$ \\sqrt{s} $$ = 13 TeV with the ATLAS detector by combining the H → ZZ* → 4ℓ and H → γγ decay channels","year":2023,"lang":"en","type":"article","venue":"Journal of High Energy Physics","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":10,"is_retracted":false,"has_abstract":true,"ca_institutions":"York University; University of British Columbia; Simon Fraser University; TRIUMF; Carleton University; University of Alberta; Université de Montréal; Institute of Particle Physics; University of Victoria; McGill University; University of Toronto","funders":"European Social Fund; Fundação para a Ciência e a Tecnologia; Institut National de Physique Nucléaire et de Physique des Particules; Agencia Nacional de Promoción Científica y Tecnológica; Science and Technology Facilities Council; Natural Sciences and Engineering Research Council of Canada; Narodowa Agencja Wymiany Akademickiej; Centre National pour la Recherche Scientifique et Technique; Centre National de la Recherche Scientifique; Israel Science Foundation; Japan Society for the Promotion of Science; Conselho Nacional de Desenvolvimento Científico e Tecnológico; Bundesministerium für Wissenschaft, Forschung und Wirtschaft; Generalitat Valenciana; Austrian Science Fund; European Regional Development Fund; Bundesministerium für Bildung und Forschung; Ministerstvo Školství, Mládeže a Tělovýchovy; U.S. Department of Energy; National Natural Science Foundation of China; Fundação de Amparo à Pesquisa do Estado de São Paulo; H2020 Marie Skłodowska-Curie Actions; Javna Agencija za Raziskovalno Dejavnost RS; Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung; Nederlandse Organisatie voor Wetenschappelijk Onderzoek; Ministry of Education, Culture, Sports, Science and Technology; Agence Nationale de la Recherche; National Science Foundation; Alexander von Humboldt-Stiftung; TRIUMF; Compute Canada; Max-Planck-Gesellschaft; Royal Society; Danmarks Grundforskningsfond; British Columbia Knowledge Development Fund; Türkiye Enerji, Nükleer ve Maden Araştırma Kurumu; Agencia Nacional de Investigación y Desarrollo; Generalitat de Catalunya; Canarie; Deutsche Forschungsgemeinschaft; Centres de Recerca de Catalunya; CERN; Leverhulme Trust; Ministerio de Ciencia e Innovación; European Commission","keywords":"Physics; Higgs boson; Particle physics; Nuclear physics","routes":{"ca_aff":true,"ca_fund":true,"ca_venue":false,"about_ca":false,"invisible_to_affiliation_only":false},"retraction":null,"screen":null,"direct_labels":[],"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.000787607,0.0005907493,0.0005236744,0.001496946,0.0002529412,0.0007587528,0.0006194477,0.0003343041,0.004288086],"category_scores_gemma":[0.0007204926,0.000463908,0.0006143335,0.00229171,0.0001962996,0.0003337233,0.0007121681,0.0002944508,0.0009749793],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.000546634,"about_ca_system_score_gemma":0.0004680839,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.004031114,"about_ca_topic_score_gemma":0.00827425,"domain_scores_codex":[0.9993826,0.00008718714,0.00003006952,0.0002018246,0.0001988958,0.00009946644],"domain_scores_gemma":[0.9992756,0.0002491371,0.000169921,0.0001160933,0.0001221828,0.00006706342],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"observational","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.002451321,0.0004305419,0.4869772,0.0004326741,0.001825829,0.0006056561,0.0002199539,0.02733298,0.4136796,0.00485292,0.01021133,0.05098002],"study_design_scores_gemma":[0.0001065612,0.0003300314,0.7422929,0.00001933895,0.0004601507,0.0005573071,0.0001179532,0.03813159,0.206233,0.001219256,0.01042931,0.0001025516],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9659684,0.0002199719,0.01121723,0.00006211177,0.0000118048,0.00002649751,0.01699231,0.0004828427,0.005018673],"genre_scores_gemma":[0.9555494,0.0002176491,0.0124188,0.00007444216,0.00002707978,0.00007221054,0.02827226,0.0001637268,0.003204536],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.004288086,"threshold_uncertainty_score":0.01434505,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01225161300503499,"score_gpt":0.2285821480502302,"score_spread":0.2163305350451952,"validation_status":"score_only:v0-immature-baseline","note":"Baseline scores from an immature model (maturity gate not passed). 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