{"id":"W4377020023","doi":"10.1016/j.physletb.2023.137963","title":"Combination of searches for invisible decays of the Higgs boson using 139 fb−1 of proton-proton collision data at s=13 TeV collected with the ATLAS experiment","year":2023,"lang":"lv","type":"article","venue":"Physics Letters B","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":86,"is_retracted":false,"has_abstract":true,"ca_institutions":"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; Particle physics; Higgs boson; Large Hadron Collider; Dark matter; Standard Model (mathematical formulation); Nuclear physics; Boson; Branching fraction; Context (archaeology); Scalar boson; Physics beyond the Standard Model","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":[0.002411231,0.0006626712,0.0009466336,0.002523344,0.0007068675,0.001379491,0.0006327608,0.0004936447,0.001648885],"category_scores_gemma":[0.001763632,0.0005258908,0.001164897,0.002559296,0.0003154264,0.000365049,0.001356072,0.0002716354,0.0004523413],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0003950982,"about_ca_system_score_gemma":0.0004897381,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.001505649,"about_ca_topic_score_gemma":0.003589748,"domain_scores_codex":[0.997247,0.0007165692,0.0002441502,0.0006691544,0.0008870657,0.0002360432],"domain_scores_gemma":[0.9977011,0.001060192,0.0004127743,0.0003313029,0.0003206447,0.0001739671],"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":[0.005926268,0.0004701388,0.7284101,0.0003931837,0.003229326,0.002036388,0.0003337766,0.008919191,0.1832932,0.001876419,0.001629187,0.06348267],"study_design_scores_gemma":[0.0002555984,0.001640564,0.6933712,0.00004795184,0.002126398,0.00640863,0.0005251917,0.03817894,0.24631,0.002103327,0.008777508,0.0002547104],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9868726,0.0004261193,0.007021163,0.00004759086,0.00002138473,0.00003797482,0.002012366,0.0001206423,0.003440109],"genre_scores_gemma":[0.9898415,0.0001564461,0.005527567,0.00002485125,0.00002094905,0.00002672139,0.003711093,0.00003189497,0.0006589412],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.002523344,"threshold_uncertainty_score":0.01275194,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02967424329715119,"score_gpt":0.2664265686787616,"score_spread":0.2367523253816105,"validation_status":"score_only:v0-immature-baseline","note":"Baseline scores from an immature model (maturity gate not passed). 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