{"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":"codex-gemma-dda1882f352a","candidate_categories":["metaepi_narrow","insufficient_payload"],"consensus_categories":[],"category_scores_codex":[0.0008190648,0.0005396269,0.0003595716,0.0001208905,0.001100218,0.0003166189,0.001287611,0.0003497161,0.001084182],"category_scores_gemma":[0.0001353284,0.0006573855,0.0007484663,0.001049943,0.001604065,0.0006154763,0.002216886,0.0005499036,0.0001213698],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00002547283,"about_ca_system_score_gemma":0.0004358902,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.00131162,"about_ca_topic_score_gemma":0.00004863868,"domain_scores_codex":[0.9952812,0.0002631882,0.001001483,0.0009540693,0.001401094,0.001098996],"domain_scores_gemma":[0.9959385,0.0008977522,0.001284831,0.001422103,0.0001858989,0.0002709514],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.002250109,0.0009822727,0.0001483996,0.001302695,0.00172471,0.00002956556,0.005128046,0.002222596,0.1713476,0.7926899,0.02135581,0.0008183361],"study_design_scores_gemma":[0.00147882,0.0009377653,0.00004971795,0.0008283365,0.0005862456,0.00001492968,0.001654934,0.1446619,0.8481583,0.0007172715,0.0003952336,0.0005165744],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9906272,0.0002339575,0.001010553,0.0009617576,0.0003456745,0.0002807591,0.0007804021,0.00006118681,0.005698461],"genre_scores_gemma":[0.9950357,0.00009518025,0.0007009826,0.0002826409,0.0007435113,0.002025857,0.0008359906,0.0002520015,0.00002815493],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.7919726,"threshold_uncertainty_score":0.9998289,"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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