{"id":"W2144382551","doi":"10.1007/jhep09(2014)015","title":"Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s $$ \\sqrt{s} $$ = 8 TeV with the ATLAS detector","year":2014,"lang":"en","type":"article","venue":"Journal of High Energy Physics","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":104,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of British Columbia; McGill University; Simon Fraser University; York University; TRIUMF; Carleton University; University of Regina; Université de Montréal; University of Victoria; University of Alberta; Institute of Particle Physics; 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; Georgian National Science Foundation; Centre National de la Recherche Scientifique; Israel Science Foundation; Lundbeckfonden; Leverhulme Trust; General Secretariat for Research and Technology; Ministry of Education, Culture, Sports, Science and Technology; Nederlandse Organisatie voor Wetenschappelijk Onderzoek; Austrian Science Fund; Bundesministerium für Bildung und Forschung; Israeli Centers for Research Excellence; Joint Institute for Nuclear Research; 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; Bundesministerium für Wissenschaft und Forschung; Javna Agencija za Raziskovalno Dejavnost RS; Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung; Ministerstwo Edukacji i Nauki; CERN; Departamento Administrativo de Ciencia, Tecnología e Innovación (COLCIENCIAS); Deutsche Forschungsgemeinschaft; National Science Foundation; Alexander von Humboldt-Stiftung; TRIUMF; Max-Planck-Gesellschaft; Royal Society; 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; Neutralino; Chargino; Branching fraction; Nuclear physics; Hadron; Pair production; Large Hadron Collider","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":[0.0009071659,0.0007795209,0.0006079362,0.0009436844,0.0005201862,0.0009603918,0.0006453395,0.0005279799,0.002660208],"category_scores_gemma":[0.0006959086,0.0004108053,0.0004241139,0.001044386,0.0002344354,0.0004409246,0.0007041788,0.0001909207,0.0005902143],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0005255082,"about_ca_system_score_gemma":0.0005106469,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.001807162,"about_ca_topic_score_gemma":0.003931372,"domain_scores_codex":[0.9995303,0.0001197626,0.00002875705,0.0001168394,0.0001037738,0.0001005426],"domain_scores_gemma":[0.9994985,0.0001930087,0.00008751182,0.00004135642,0.00006199141,0.0001176693],"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":[0.01083197,0.0007067214,0.5426263,0.0005340768,0.001352731,0.008221245,0.0004069681,0.005783908,0.4023519,0.005578835,0.002363466,0.01924198],"study_design_scores_gemma":[0.0009935468,0.006983632,0.4456541,0.00003069138,0.0009607742,0.009987152,0.0004525197,0.04173212,0.483506,0.003690547,0.005814975,0.0001939359],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9939548,0.0002681109,0.002295605,0.00002976837,0.000004873319,0.00003052585,0.001188821,0.0001170064,0.002110529],"genre_scores_gemma":[0.9944544,0.00005904687,0.002268089,0.00001785838,0.000005127946,0.00001206635,0.002365041,0.000008968646,0.0008094473],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.002660208,"threshold_uncertainty_score":0.008899331,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01549003995360225,"score_gpt":0.2610385505299446,"score_spread":0.2455485105763424,"validation_status":"score_only:v0-immature-baseline","note":"Baseline scores from an immature model (maturity gate not passed). 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