{"id":"W2102604073","doi":"10.1103/physrevlett.108.211803","title":"Evidence for the Charmless Annihilation Decay Mode<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msubsup><mml:mi>B</mml:mi><mml:mi>s</mml:mi><mml:mn>0</mml:mn></mml:msubsup><mml:mo>→</mml:mo><mml:msup><mml:mi>π</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>π</mml:mi><mml:mo>−</mml:mo></mml:msup></mml:math>","year":2012,"lang":"lv","type":"article","venue":"Physical Review Letters","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":43,"is_retracted":false,"has_abstract":true,"ca_institutions":"","funders":"Fermilab; Alfred P. Sloan Foundation; National Science Council; Natural Sciences and Engineering Research Council of Canada; Istituto Nazionale di Fisica Nucleare; Science and Technology Facilities Council; National Research Foundation; National Research Foundation of Korea; Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung; U.S. Department of Energy; Russian Foundation for Basic Research; Ministry of Education, Culture, Sports, Science and Technology; National Science Foundation","keywords":"Physics; Annihilation; Particle physics; Tevatron; Hadron; Luminosity; Branching fraction; Electron–positron annihilation; Collider Detector at Fermilab; Nuclear physics; Astrophysics; Large Hadron Collider","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":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0004984895,0.0004025385,0.0002827389,0.001730023,0.000694846,0.0006777601,0.0004918248,0.000500872,0.007272276],"category_scores_gemma":[0.0007506637,0.0003239413,0.0003427428,0.001765059,0.0002722717,0.0003423969,0.0006500156,0.0003510027,0.001625156],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0003697464,"about_ca_system_score_gemma":0.000374394,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.00325432,"about_ca_topic_score_gemma":0.005767999,"domain_scores_codex":[0.9996147,0.00004382015,0.0000343668,0.00009823409,0.0001019689,0.0001069357],"domain_scores_gemma":[0.9992963,0.0002245489,0.0001527187,0.0000902157,0.00009216506,0.000143946],"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":[0.002695849,0.0004168793,0.6238112,0.0002500748,0.000201508,0.003088504,0.0007962012,0.0008763385,0.3139104,0.008510422,0.005838503,0.0396041],"study_design_scores_gemma":[0.0002224765,0.0008177292,0.5772592,0.00004413093,0.0001704531,0.005811262,0.0006779452,0.005024442,0.3842174,0.003011393,0.02263734,0.0001063004],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9892749,0.0001511391,0.002008196,0.0000937471,0.00000805656,0.00003526752,0.003070013,0.0001619167,0.005196756],"genre_scores_gemma":[0.9890295,0.00008193853,0.003847485,0.00005931254,0.000004858655,0.00002482925,0.004758691,0.00002821382,0.002165154],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.007272276,"threshold_uncertainty_score":0.02432817,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.03043156308357844,"score_gpt":0.2835726543291353,"score_spread":0.2531410912455568,"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."}}