{"id":"W1528176850","doi":"10.1103/physrevlett.106.181802","title":"Measurements of Direct<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>C</mml:mi><mml:mi>P</mml:mi></mml:math>Violating Asymmetries in Charmless Decays of Strange Bottom Mesons and Bottom Baryons","year":2011,"lang":"en","type":"article","venue":"Physical Review Letters","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":62,"is_retracted":false,"has_abstract":true,"ca_institutions":"McGill University; Institute of Particle Physics; Simon Fraser University; University of Toronto; TRIUMF","funders":"Science and Technology Facilities Council; National Science Foundation","keywords":"Particle physics; Physics; CP violation; Tevatron; Hadron; Collider Detector at Fermilab; Baryon; Luminosity; Meson; Nuclear physics; Fermilab; Analytical Chemistry (journal); Large Hadron Collider","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":"codex-gemma-dda1882f352a","candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.0003216141,0.0002479997,0.0003343371,0.00003695963,0.0001758908,0.0000421711,0.0002716613,0.00004571788,0.00007475844],"category_scores_gemma":[0.00006641999,0.0002793409,0.0003651609,0.0002631586,0.0004307099,0.0002331038,0.0002797233,0.0002765845,0.00006529994],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00000637836,"about_ca_system_score_gemma":0.00004093872,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0004152285,"about_ca_topic_score_gemma":0.000009352636,"domain_scores_codex":[0.9981624,0.00009877791,0.0004901266,0.0003656127,0.000435573,0.0004474593],"domain_scores_gemma":[0.9989223,0.0002428613,0.0003115463,0.0003361037,0.0000326811,0.0001545317],"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":[0.00006957154,0.0003724264,0.001246792,0.0005840425,0.0003343316,0.000007584198,0.001062592,0.00001182217,0.02058845,0.9735975,0.0001967072,0.001928139],"study_design_scores_gemma":[0.001120514,0.0004465413,0.002117534,0.003478647,0.000814766,0.000004997096,0.0006592308,0.02344459,0.9618013,0.00514776,0.0001861698,0.0007779348],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9936382,0.0016149,0.0001577537,0.0002701957,0.0000901649,0.0000584577,0.00006916293,0.00002025198,0.004080964],"genre_scores_gemma":[0.9983426,0.0003127877,0.0005727294,0.0003301872,0.0001824596,0.0001713365,0.00003835192,0.00004832348,0.000001170829],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.9684498,"threshold_uncertainty_score":0.9999658,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.03255632833558354,"score_gpt":0.2728962921387809,"score_spread":0.2403399638031974,"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."}}