{"id":"W1870689982","doi":"10.1007/jhep11(2012)138","title":"Search for high-mass resonances decaying to dilepton final states in pp collisions at $ \\sqrt{s}=7 $ TeV with the ATLAS detector","year":2012,"lang":"en","type":"article","venue":"Journal of High Energy Physics","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":80,"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; Institute of Particle Physics; University of Regina; McGill University; University of Victoria","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; Joint Institute for Nuclear Research; 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; Japan Society for the Promotion of Science; Conselho Nacional de Desenvolvimento Científico e Tecnológico; 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; Ministerio de Ciencia e Innovación; European Commission; National Science Foundation; Alexander von Humboldt-Stiftung; TRIUMF; Max-Planck-Gesellschaft; Royal Society; Departamento Administrativo de Ciencia, Tecnología e Innovación (COLCIENCIAS); Deutsche Forschungsgemeinschaft; Ministerstwo Edukacji i Nauki; CERN; Comisión Nacional de Investigación Científica y Tecnológica; Danmarks Grundforskningsfond; Services Fédéraux des Affaires Scientifiques, Techniques et Culturelles; Department of Science and Technology, Ministry of Science and Technology, India; Türkiye Atom Enerjisi Kurumu","keywords":"Physics; Particle physics; Boson; Graviton; Randall–Sundrum model; Gauge boson; Muon; Nuclear physics; Large Hadron Collider; Gauge theory; Gravitation; Brane; Theoretical physics; Quantum mechanics","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":[0.001116409,0.0005099134,0.0005745624,0.001778513,0.0009202505,0.001141615,0.0005757526,0.0005760674,0.002422682],"category_scores_gemma":[0.0009494197,0.0004037709,0.0003633958,0.001455047,0.0002724656,0.0003747041,0.0007065736,0.0002891143,0.0004596636],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0005190386,"about_ca_system_score_gemma":0.000378163,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.00139185,"about_ca_topic_score_gemma":0.002458388,"domain_scores_codex":[0.9994849,0.0001784195,0.00002902963,0.0001091406,0.000100095,0.00009834196],"domain_scores_gemma":[0.9993363,0.0003423489,0.0001045316,0.00005377001,0.0000684731,0.00009452496],"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":[0.005335027,0.0005069341,0.4374682,0.0003423129,0.0005644585,0.006989306,0.0008263493,0.01790252,0.4741528,0.0281468,0.001847715,0.02591758],"study_design_scores_gemma":[0.0005813183,0.002313772,0.3433852,0.00005050472,0.0006923507,0.006246823,0.0008071744,0.1166857,0.5119582,0.01003127,0.00701759,0.0002301498],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9887488,0.000149772,0.006670996,0.00004654683,0.000005055081,0.00001555122,0.0004284684,0.0001179769,0.003816951],"genre_scores_gemma":[0.9940313,0.0000505763,0.004264329,0.00002727497,0.000005825542,0.00001285199,0.0007027328,0.00001761364,0.0008875525],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.002422682,"threshold_uncertainty_score":0.008104682,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01812223295617973,"score_gpt":0.2698006753362572,"score_spread":0.2516784423800775,"validation_status":"score_only:v0-immature-baseline","note":"Baseline scores from an immature model (maturity gate not passed). 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