{"id":"W1501840479","doi":"10.1016/j.physletb.2012.09.016","title":"Search for a standard model Higgs boson in the H→ZZ→ℓ+ℓ−νν¯ decay channel using 4.7 fb−1 of s=7 TeV data with the ATLAS detector","year":2012,"lang":"lv","type":"article","venue":"Physics Letters B","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":19,"is_retracted":false,"has_abstract":true,"ca_institutions":"Simon Fraser University; Carleton University; TRIUMF; York University; University of British Columbia; University of Alberta; Université de Montréal; University of Regina; McGill University; University of Victoria; University of Toronto","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; H. Lundbeck A/S; State Atomic Energy Corporation ROSATOM; 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; Lundbeckfonden; Leverhulme Trust; General Secretariat for Research and Technology; Ministry of Education, Culture, Sports, Science and Technology; Nederlandse Organisatie voor Wetenschappelijk Onderzoek; Bundesministerium für Bildung und Forschung; National Science Council; U.S. Department of Energy; National Natural Science Foundation of China; Fundação de Amparo à Pesquisa do Estado de São Paulo; Bundesministerium für Wissenschaft und Forschung; Javna Agencija za Raziskovalno Dejavnost RS; Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung; National Science Foundation; Alexander von Humboldt-Stiftung; TRIUMF; Max-Planck-Gesellschaft; American Roentgen Ray Society; Royal Society; Joint Institute for Nuclear Research; Arizona-Nevada Academy of Science; Services Fédéraux des Affaires Scientifiques, Techniques et Culturelles; Department of Science and Technology, Ministry of Science and Technology, India; Türkiye Atom Enerjisi Kurumu; Departamento Administrativo de Ciencia, Tecnología e Innovación (COLCIENCIAS); Deutsche Forschungsgemeinschaft; Ministerstwo Edukacji i Nauki; CERN; Comisión Nacional de Investigación Científica y Tecnológica; Danmarks Grundforskningsfond; Ministerio de Ciencia e Innovación; European Commission","keywords":"Higgs boson; Physics; Particle physics; Standard Model (mathematical formulation); Large Hadron Collider; Muon; Boson; Nuclear physics; Luminosity; 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":[0.0004123136,0.0004547295,0.0005197701,0.001151926,0.0007965876,0.001045561,0.0005120363,0.001074192,0.02372625],"category_scores_gemma":[0.0004583339,0.0004478183,0.001101102,0.001235688,0.0001834194,0.0005888304,0.000601725,0.000525199,0.005525239],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0004654568,"about_ca_system_score_gemma":0.0004302268,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.002703637,"about_ca_topic_score_gemma":0.0053552,"domain_scores_codex":[0.9998547,0.00001545279,0.000004514623,0.00003986632,0.00003566465,0.00004980036],"domain_scores_gemma":[0.999809,0.00004937819,0.00003188354,0.00002642228,0.00003376111,0.0000495663],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"bench_or_experimental","study_design_gemma":"observational","study_design_scores_codex":[0.01011426,0.001187053,0.1883163,0.00132398,0.001150889,0.01473883,0.001916592,0.008568269,0.3267078,0.1380242,0.1649899,0.142962],"study_design_scores_gemma":[0.004364057,0.002471728,0.2337454,0.0002905393,0.001561121,0.00564069,0.003478814,0.2025566,0.2782213,0.1177807,0.1495033,0.0003857862],"study_design_candidate":"observational","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.8670217,0.0004343401,0.02737415,0.001736686,0.0002222098,0.0001181145,0.01011564,0.003375952,0.08960111],"genre_scores_gemma":[0.9443204,0.0001206733,0.01369608,0.0004698132,0.00004945994,0.00006074517,0.009572927,0.0005203633,0.03118943],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.02372625,"threshold_uncertainty_score":0.07937223,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02502662441952031,"score_gpt":0.2557666352370144,"score_spread":0.2307400108174941,"validation_status":"score_only:v0-immature-baseline","note":"Baseline scores from an immature model (maturity gate not passed). 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