{"id":"W2338527021","doi":"10.1007/jhep05(2016)160","title":"Search for the Standard Model Higgs boson decaying into b b ¯ $$ b\\overline{b} $$ produced in association with top quarks decaying hadronically in pp collisions at s = 8 $$ \\sqrt{s}=8 $$ TeV with the ATLAS detector","year":2016,"lang":"en","type":"article","venue":"Journal of High Energy Physics","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":39,"is_retracted":false,"has_abstract":true,"ca_institutions":"Simon Fraser University; University of British Columbia; York University; TRIUMF; Carleton University; University of Victoria; McGill University; University of Toronto; University of Alberta; Université de Montréal; Institute of Particle Physics","funders":"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; Max-Planck-Gesellschaft; Israel Science Foundation; Israeli Centers for Research Excellence; Joint Institute for Nuclear Research; Centre National pour la Recherche Scientifique et Technique; Bundesministerium für Wissenschaft, Forschung und Wirtschaft; General Secretariat for Research and Technology; Ministry of Education, Culture, Sports, Science and Technology; Nederlandse Organisatie voor Wetenschappelijk Onderzoek; Bundesministerium für Bildung und Forschung; Fundação de Amparo à Pesquisa do Estado de São Paulo; Javna Agencija za Raziskovalno Dejavnost RS; Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung; Ministerstwo Edukacji i Nauki; CERN; Austrian Science Fund; Comisión Nacional de Investigación Científica y Tecnológica; Danmarks Grundforskningsfond; National Research Center \"Kurchatov Institute\"; Centre National de la Recherche Scientifique; Türkiye Atom Enerjisi Kurumu; Japan Society for the Promotion of Science; Conselho Nacional de Desenvolvimento Científico e Tecnológico; National Natural Science Foundation of China; Georgian National Science Foundation; Services Fédéraux des Affaires Scientifiques, Techniques et Culturelles; Department of Science and Technology, Ministry of Science and Technology, India; Departamento Administrativo de Ciencia, Tecnología e Innovación (COLCIENCIAS)","keywords":"Physics; Particle physics; Higgs boson; Standard Model (mathematical formulation); Top quark; Boson; Quark; Luminosity; Branching fraction; Large Hadron Collider; Nuclear physics; Hadron; Bottom quark; 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":[0.0005959083,0.0004420077,0.0004852587,0.001148719,0.0003377443,0.0008290499,0.0004762137,0.0004035236,0.001751457],"category_scores_gemma":[0.0004330897,0.0003095649,0.0003694003,0.001235806,0.0001692766,0.0002745115,0.0004723227,0.0001690119,0.0004570416],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0002260607,"about_ca_system_score_gemma":0.000483099,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0007897919,"about_ca_topic_score_gemma":0.001359914,"domain_scores_codex":[0.9996778,0.00006706904,0.00001710845,0.00007986087,0.0001035317,0.00005459382],"domain_scores_gemma":[0.9996272,0.0001157873,0.0000910169,0.00003270736,0.00004989484,0.00008326841],"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":[0.00375452,0.0005573347,0.4497066,0.0002335368,0.0005700465,0.003220069,0.0002100828,0.005463634,0.5001721,0.006480839,0.001600923,0.02803011],"study_design_scores_gemma":[0.0004576474,0.002161941,0.4012743,0.00002975736,0.0007386333,0.00559441,0.0004361504,0.0997586,0.4799438,0.004349748,0.005132141,0.0001228493],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9942183,0.0001023085,0.003853374,0.00002218705,0.000003681838,0.00001164445,0.0002764716,0.00008987085,0.0014221],"genre_scores_gemma":[0.992167,0.0000611444,0.005894478,0.00001995972,0.000005557073,0.000009232762,0.001036827,0.00001352376,0.0007923229],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.001751457,"threshold_uncertainty_score":0.005859196,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01114580769868797,"score_gpt":0.2581130931916626,"score_spread":0.2469672854929747,"validation_status":"score_only:v0-immature-baseline","note":"Baseline scores from an immature model (maturity gate not passed). 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