{"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":"codex-gemma-dda1882f352a","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0002801235,0.0001419598,0.0002843908,0.00002313898,0.000133567,0.00001694513,0.0002069802,0.00001758812,0.000006046503],"category_scores_gemma":[0.000008011709,0.00007162377,0.0001245819,0.0002578923,0.0001966728,0.0001091595,0.00009146945,0.0001583337,7.184008e-7],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00007956977,"about_ca_system_score_gemma":0.00004897863,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0001920534,"about_ca_topic_score_gemma":0.00001456487,"domain_scores_codex":[0.9989068,0.0001434069,0.0002909454,0.0001440789,0.0002639341,0.0002508168],"domain_scores_gemma":[0.9992417,0.0002000964,0.0002222921,0.0001832836,0.0001137069,0.00003892483],"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":[0.003445133,0.002940388,0.3601567,0.0001650856,0.0006155603,0.000001547195,0.003862698,0.07926293,0.06577798,0.4701705,0.0004642973,0.01313723],"study_design_scores_gemma":[0.0008892734,0.0004063822,0.001607049,0.00008418355,0.00002731135,4.750192e-7,0.0002452969,0.0006752602,0.9302217,0.06482962,0.000910574,0.000102921],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9968106,0.00004051351,0.001657785,0.0008424783,0.0000746384,0.0004634626,0.000008558123,0.000002919932,0.00009906445],"genre_scores_gemma":[0.9993343,0.000005600067,0.000117282,0.00001015198,0.0002692846,0.0002107639,0.00000297604,0.00001480078,0.00003485039],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.8644437,"threshold_uncertainty_score":0.2920732,"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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