{"id":"W2153424170","doi":"10.1103/physrevlett.92.201802","title":"Measurements of Branching Fractions and<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<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>B</mml:mi></mml:math>Meson Decays to Charmless Two-Body States Containing a<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>K</mml:mi><mml:mn>0</mml:mn></mml:msup></mml:math>","year":2004,"lang":"lv","type":"article","venue":"Physical Review Letters","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":14,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of Victoria; Université de Montréal; McGill University; University of British Columbia","funders":"Institut National de Physique Nucléaire et de Physique des Particules; Institute of High Energy Physics; Natural Sciences and Engineering Research Council of Canada; Centre National de la Recherche Scientifique; Bundesministerium für Bildung und Forschung; SLAC National Accelerator Laboratory; Alexander von Humboldt-Stiftung; Alfred P. Sloan Foundation; Deutsche Forschungsgemeinschaft; U.S. Department of Energy; National Science Foundation","keywords":"Physics; Particle physics; Branching fraction; B meson; Meson; Electron–positron annihilation; Combinatorics; Hadron; Mathematics","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":[0.0005033639,0.0007095209,0.000316221,0.001804422,0.000706134,0.0007877459,0.0005431033,0.0005853203,0.005650036],"category_scores_gemma":[0.0008709311,0.000443226,0.0004024541,0.001163076,0.0002593421,0.0005347002,0.0006106787,0.0004319869,0.001591219],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00038596,"about_ca_system_score_gemma":0.0001608998,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.00202209,"about_ca_topic_score_gemma":0.004207795,"domain_scores_codex":[0.999507,0.00006750964,0.00002946804,0.0001475549,0.0001427804,0.0001058494],"domain_scores_gemma":[0.9993184,0.00024608,0.0001394853,0.000120982,0.0001117779,0.0000633721],"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":[0.002055472,0.0009449975,0.3060366,0.0002957181,0.0003467873,0.0008142946,0.0008986067,0.005961091,0.6017489,0.006300917,0.003089699,0.07150696],"study_design_scores_gemma":[0.0001213015,0.000627885,0.2083892,0.0000442773,0.0001531107,0.001143286,0.0002598995,0.0125428,0.7670786,0.001711514,0.007815599,0.0001125456],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9812407,0.0001831133,0.005451794,0.00003400085,0.000006856996,0.00003689765,0.003528234,0.0002765351,0.009241822],"genre_scores_gemma":[0.9844567,0.0002781026,0.004997957,0.00003813253,0.000008477077,0.00004641913,0.007150752,0.00008615702,0.002937289],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.005650036,"threshold_uncertainty_score":0.01890129,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02205560333987026,"score_gpt":0.2750831704715494,"score_spread":0.2530275671316791,"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."}}