{"id":"W2105486687","doi":"10.1016/j.nima.2012.10.079","title":"Pion emission from the T2K replica target: Method, results and application","year":2012,"lang":"en","type":"article","venue":"Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment","topic":"Neutrino Physics Research","field":"Physics and Astronomy","cited_by":41,"is_retracted":false,"has_abstract":false,"ca_institutions":"University of Toronto","funders":"Institut National de Physique Nucléaire et de Physique des Particules; Hungarian Scientific Research Fund; Ministry of Education, Culture, Sports, Science and Technology; Ministry of Education and Science of the Russian Federation; European Regional Development Fund; European Commission; Fundacja na rzecz Nauki Polskiej; Japan Society for the Promotion of Science; Russian Foundation for Basic Research; CERN; Deutsche Forschungsgemeinschaft; Ministerio de Educación, Cultura y Deporte","keywords":"Physics; Neutrino; Nuclear physics; Neutrino oscillation; Large Hadron Collider; Flux (metallurgy); Particle physics; Hadron; Pion; Proton; Solar neutrino problem; Solar neutrino","routes":{"ca_aff":true,"ca_fund":false,"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":[0.0009440194,0.000589936,0.0006125885,0.0005455792,0.0005908929,0.0009989548,0.001266973,0.0007663096,0.005797572],"category_scores_gemma":[0.0009473036,0.0002722143,0.0004077975,0.001043251,0.0005796429,0.0009353707,0.0009639023,0.0006766407,0.001400158],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0004777755,"about_ca_system_score_gemma":0.0003482371,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0007748263,"about_ca_topic_score_gemma":0.0004818796,"domain_scores_codex":[0.999517,0.0001644985,0.00001248229,0.00009030588,0.0001730327,0.00004266561],"domain_scores_gemma":[0.9994357,0.0002031192,0.00004874596,0.0001822126,0.00009210305,0.00003807797],"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":[0.004257289,0.0006444533,0.0138273,0.001928834,0.000228137,0.001823338,0.001565491,0.07456996,0.595721,0.104615,0.002276645,0.1985427],"study_design_scores_gemma":[0.0002683402,0.0008009998,0.005934254,0.00008550093,0.0001442553,0.001468189,0.0003993883,0.3530815,0.6145853,0.01650996,0.00648718,0.000235101],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.5530112,0.001933167,0.384681,0.0004900356,0.0001177223,0.0003128646,0.0008665403,0.00205274,0.05653477],"genre_scores_gemma":[0.9233884,0.0009593449,0.06507259,0.00006371649,0.00003161576,0.0001524197,0.0002911235,0.0004631399,0.009577649],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.005797572,"threshold_uncertainty_score":0.01939481,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.04578686756848868,"score_gpt":0.3999735281857078,"score_spread":0.3541866606172192,"validation_status":"score_only:v0-immature-baseline","note":"Baseline scores from an immature model (maturity gate not passed). Scores rank; they never assert a category."}}