{"id":"W4388743511","doi":"10.1007/jhep02(2024)128","title":"Search for resonant production of dark quarks in the dijet final state with the ATLAS detector","year":2024,"lang":"en","type":"article","venue":"Journal of High Energy Physics","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":8,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of British Columbia; York University; Institute of Particle Physics; University of Toronto; Carleton University; Simon Fraser University; University of Alberta; Université de Montréal; University of Victoria; McGill University","funders":"European Social Fund; 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; Narodowa Agencja Wymiany Akademickiej; 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; Bundesministerium für Wissenschaft, Forschung und Wirtschaft; Generalitat Valenciana; Austrian Science Fund; European Regional Development Fund; Bundesministerium für Bildung und Forschung; Ministerstvo Školství, Mládeže a Tělovýchovy; U.S. Department of Energy; National Natural Science Foundation of China; Fundação de Amparo à Pesquisa do Estado de São Paulo; H2020 Marie Skłodowska-Curie Actions; Javna Agencija za Raziskovalno Dejavnost RS; Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung; Nederlandse Organisatie voor Wetenschappelijk Onderzoek; Ministry of Education, Culture, Sports, Science and Technology; Agence Nationale de la Recherche; National Science Foundation; Alexander von Humboldt-Stiftung; TRIUMF; Compute Canada; Max-Planck-Gesellschaft; Royal Society; Danmarks Grundforskningsfond; British Columbia Knowledge Development Fund; Türkiye Enerji, Nükleer ve Maden Araştırma Kurumu; Agencia Nacional de Investigación y Desarrollo; Generalitat de Catalunya; Canarie; Deutsche Forschungsgemeinschaft; Centres de Recerca de Catalunya; CERN; Leverhulme Trust; Ministerio de Ciencia e Innovación; European Commission","keywords":"Physics; Particle physics; Quark; Hadron; Invariant mass; Large Hadron Collider; Branching fraction; Nuclear physics; ATLAS experiment; Atlas (anatomy); Standard Model (mathematical formulation); Dark matter","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":[0.0008240855,0.0003183168,0.0003053088,0.001630785,0.0004664544,0.001017323,0.0005195827,0.0003293699,0.003171889],"category_scores_gemma":[0.0007787388,0.0002483352,0.0003277955,0.001292131,0.0001736011,0.0003735446,0.0006312567,0.0001963073,0.0005303685],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0005939176,"about_ca_system_score_gemma":0.000425418,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.002306303,"about_ca_topic_score_gemma":0.004629799,"domain_scores_codex":[0.9995733,0.00008724827,0.00002408417,0.00009273299,0.0001205382,0.0001020424],"domain_scores_gemma":[0.9993994,0.0002214453,0.0001523374,0.00006713054,0.00007956591,0.00008006509],"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":[0.003680925,0.0002965224,0.6461679,0.0002478603,0.0004032713,0.002723052,0.0003994577,0.007694739,0.2873411,0.0150778,0.002210151,0.03375728],"study_design_scores_gemma":[0.0002582619,0.001551045,0.3265111,0.00004178599,0.0005766401,0.003941149,0.0009062526,0.1253514,0.5164678,0.008224255,0.01595086,0.0002194304],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9775072,0.0002565484,0.0142882,0.00003595951,0.000011622,0.00002441976,0.001478661,0.0003600613,0.006037367],"genre_scores_gemma":[0.9923523,0.00004675324,0.005504554,0.00001705426,0.000004133188,0.000008948971,0.001148897,0.00001768612,0.0008996025],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.003171889,"threshold_uncertainty_score":0.01061106,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01591671859457856,"score_gpt":0.2649103720698782,"score_spread":0.2489936534752997,"validation_status":"score_only:v0-immature-baseline","note":"Baseline scores from an immature model (maturity gate not passed). 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