{"id":"W2317468123","doi":"10.1142/s0217751x01007212","title":"SEARCH FOR THE DECAY B<sub>s</sub>→μ<sup>+</sup>μ <sup>-</sup>ϕ IN $p\\bar p$ COLLISIONS AT $\\sqrt{s} =1.8\\, {\\rm TeV}$","year":2001,"lang":"en","type":"article","venue":"International Journal of Modern Physics A","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":0,"is_retracted":false,"has_abstract":true,"ca_institutions":"","funders":"National Science Council; Fermilab; U.S. Department of Energy; Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung; Natural Sciences and Engineering Research Council of Canada; Istituto Nazionale di Fisica Nucleare; Alfred P. Sloan Foundation","keywords":"Physics; Collider Detector at Fermilab; Branching fraction; Particle physics; Collider; Fermilab; Bar (unit); Nuclear physics; Particle decay; Tevatron; Boson; 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":"codex-gemma-dda1882f352a","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0003549662,0.000289439,0.0003914459,0.00007743641,0.0002881178,0.0001339876,0.0007541571,0.00004562164,0.00006335826],"category_scores_gemma":[0.0000170062,0.0002153781,0.0004397357,0.0002029277,0.0002453716,0.0003427234,0.0003642897,0.0003757255,0.00006411139],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0002417113,"about_ca_system_score_gemma":0.0000981273,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.00005160495,"about_ca_topic_score_gemma":0.000001191035,"domain_scores_codex":[0.9977221,0.00008226182,0.0006189109,0.000285087,0.0008083982,0.0004832368],"domain_scores_gemma":[0.9982525,0.0006101556,0.0002303284,0.0002312388,0.0005043948,0.0001714392],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"simulation_or_modeling","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.001816969,0.002904051,0.07411861,0.00001553709,0.002191543,0.000052429,0.00914379,0.4698848,0.07952441,0.2456136,0.001885824,0.1128485],"study_design_scores_gemma":[0.003414161,0.0002281828,0.0006148445,0.0001533795,0.0001083087,0.00002402031,0.001758498,0.2963561,0.4893201,0.2052602,0.00230251,0.0004596966],"study_design_candidate":"simulation_or_modeling","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9561535,0.0002520891,0.03953341,0.002066183,0.0001604354,0.0002716469,0.0001074756,0.00001079743,0.001444528],"genre_scores_gemma":[0.9978614,0.00009579265,0.0002680644,0.00009763566,0.00149909,0.00006000042,0.00002085256,0.00004116527,0.00005602599],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.4097957,"threshold_uncertainty_score":0.8782862,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02535203372324143,"score_gpt":0.3043359562729834,"score_spread":0.278983922549742,"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."}}