{"id":"W4380364246","doi":"10.1016/j.physletb.2023.137880","title":"Measurement of the Higgs boson mass in the H → ZZ⁎ → 4ℓ decay channel using 139 fb−1 of s=13 TeV pp collisions recorded by the ATLAS detector at the LHC","year":2023,"lang":"lv","type":"article","venue":"Physics Letters B","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":14,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of Toronto","funders":"H2020 Marie Skłodowska-Curie Actions; Institut National de Physique Nucléaire et de Physique des Particules; Fundação para a Ciência e a Tecnologia; Agencia Nacional de Promoción Científica y Tecnológica; Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung; Science and Technology Facilities Council; Bundesministerium für Bildung und Forschung; Ministry of Education, Culture, Sports, Science and Technology; Natural Sciences and Engineering Research Council of Canada; Narodowa Agencja Wymiany Akademickiej; European Social Fund; Royal Society; Centre National pour la Recherche Scientifique et Technique; Japan Society for the Promotion of Science; National Research Center \"Kurchatov Institute\"; European Regional Development Fund; Max-Planck-Gesellschaft; British Columbia Knowledge Development Fund; Centre National de la Recherche Scientifique; Knut och Alice Wallenbergs Stiftelse; Israel Science Foundation; Türkiye Atom Enerjisi Kurumu; Joint Institute for Nuclear Research; Conselho Nacional de Desenvolvimento Científico e Tecnológico; Bundesministerium für Wissenschaft, Forschung und Wirtschaft; Generalitat de Catalunya; Generalitat Valenciana; Agencia Nacional de Investigación y Desarrollo; Services Fédéraux des Affaires Scientifiques, Techniques et Culturelles; Austrian Science Fund; U.S. Department of Energy; National Natural Science Foundation of China; Leverhulme Trust; European Commission; Fundação de Amparo à Pesquisa do Estado de São Paulo; Javna Agencija za Raziskovalno Dejavnost RS; Deutsche Forschungsgemeinschaft; Nederlandse Organisatie voor Wetenschappelijk Onderzoek; Agence Nationale de la Recherche; Danmarks Grundforskningsfond; TRIUMF; Alexander von Humboldt-Stiftung; Türkiye Enerji, Nükleer ve Maden Araştırma Kurumu; National Science Foundation; Compute Canada; Ministerstvo Školství, Mládeže a Tělovýchovy; Canarie; CERN; Centres de Recerca de Catalunya; Ministerio de Ciencia e Innovación","keywords":"Physics; Higgs boson; Particle physics; Luminosity; Large Hadron Collider; Standard Model (mathematical formulation); Nuclear physics; Muon; Lepton; Invariant mass; Electron; Astrophysics","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":[0.001041783,0.0008296015,0.0005087148,0.001948068,0.0006937095,0.0008765695,0.0007731233,0.0005950769,0.007110678],"category_scores_gemma":[0.0006552409,0.0005471363,0.0007425506,0.002243112,0.0003610372,0.0005108239,0.0009279546,0.0004323159,0.002100272],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0007213507,"about_ca_system_score_gemma":0.0005190278,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.002949655,"about_ca_topic_score_gemma":0.005438109,"domain_scores_codex":[0.9992563,0.00007250017,0.00002841087,0.000277402,0.0002594564,0.0001058803],"domain_scores_gemma":[0.9995446,0.0001163081,0.0001301036,0.0001001735,0.00007160418,0.00003716803],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"bench_or_experimental","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.003102302,0.0008626496,0.3517242,0.0005838672,0.001541313,0.001568442,0.0005251764,0.004397199,0.5474126,0.008842035,0.01223499,0.06720521],"study_design_scores_gemma":[0.0002193228,0.00079966,0.4048349,0.00007818204,0.0005940297,0.001934005,0.0002707089,0.01275845,0.5389428,0.002128885,0.03726766,0.0001715084],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9201149,0.0005706027,0.03058562,0.0001555372,0.00008832797,0.0001478836,0.02491048,0.001866585,0.02156018],"genre_scores_gemma":[0.9411002,0.0003425138,0.02347788,0.0001299309,0.00004375975,0.0001322446,0.03028623,0.0002790619,0.004208202],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.007110678,"threshold_uncertainty_score":0.02378762,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02149931439262228,"score_gpt":0.2407883971221472,"score_spread":0.2192890827295249,"validation_status":"score_only:v0-immature-baseline","note":"Baseline scores from an immature model (maturity gate not passed). 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