{"id":"W2483284319","doi":"10.1103/physrevd.94.011101","title":"Tests of CPT symmetry in B^0-Bbar^0 mixing and in B^0 → ccbarK^0 decays","year":2016,"lang":"en","type":"article","venue":"CaltechAUTHORS (California Institute of Technology)","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":1,"is_retracted":false,"has_abstract":true,"ca_institutions":"","funders":"SLAC National Accelerator Laboratory; Institut National de Physique Nucléaire et de Physique des Particules; Centre National de la Recherche Scientifique; Science and Technology Facilities Council; Eidgenössische Technische Hochschule Zürich; Bundesministerium für Bildung und Forschung; Alfred P. Sloan Foundation; Natural Sciences and Engineering Research Council of Canada; U.S. Department of Energy; European Commission; CERN; Deutsche Forschungsgemeinschaft; National Science Foundation","keywords":"Mixing (physics); Physics; Symmetry (geometry); CPT symmetry; Analytical Chemistry (journal); Atomic physics; Chemistry; Mathematics; Quantum mechanics; Chromatography","routes":{"ca_aff":false,"ca_fund":true,"ca_venue":false,"about_ca":false,"invisible_to_affiliation_only":true},"retraction":null,"screen":null,"direct_labels":[],"prediction":{"model_version":"codex-gemma-dda1882f352a","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0001774672,0.0001822628,0.0004331688,0.0003245836,0.00003979361,0.000003965699,0.0002159802,0.0001115869,0.00001960821],"category_scores_gemma":[0.00006767794,0.0001350568,0.00005871444,0.0006493742,0.000942888,0.0001130401,0.0002781391,0.0001652354,0.00001430985],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00003823161,"about_ca_system_score_gemma":0.00002396313,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.00008966779,"about_ca_topic_score_gemma":0.00001121234,"domain_scores_codex":[0.9987748,0.00001586234,0.0004713209,0.0002888217,0.0001112147,0.0003380317],"domain_scores_gemma":[0.9994912,0.00004863113,0.0001250092,0.000238608,0.00003601591,0.00006052648],"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":[0.00004440936,0.0002617547,0.3689846,0.00003308782,0.00002855105,0.0000044659,0.00005150374,0.000004846483,0.2366462,0.3486828,0.00001250089,0.04524529],"study_design_scores_gemma":[0.001005444,0.00007269163,0.004445135,0.000340194,0.00001152145,0.000001181884,0.0002157458,0.00006861686,0.7679254,0.2251039,0.0006115559,0.0001986066],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9959337,0.0002705469,0.001472728,0.0006930018,0.00007114879,0.0001752603,0.00006334756,0.0000362275,0.001284009],"genre_scores_gemma":[0.9982201,0.00002264669,0.00166732,0.00000634824,0.00001868915,0.00004383396,0.000001934961,0.00001211617,0.000006989856],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.5312791,"threshold_uncertainty_score":0.5507458,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01022933310332993,"score_gpt":0.2565301701533979,"score_spread":0.246300837050068,"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."}}