{"id":"W2114894457","doi":"10.1016/s0370-2693(00)00971-0","title":"A measurement of the rate of charm production in W decays","year":2000,"lang":"en","type":"article","venue":"Physics Letters B","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":7,"is_retracted":false,"has_abstract":false,"ca_institutions":"University of Victoria; University of Alberta; Université de Montréal; Carleton University; TRIUMF; University of British Columbia","funders":"Hungarian Scientific Research Fund; Bundesministerium für Bildung und Forschung; High Energy Physics; U.S. Department of Energy; Japan Society for the Promotion of Science; Ministry of Education, Culture, Sports, Science and Technology; National Science Foundation","keywords":"Physics; Particle physics; Lepton; Hadron; Nuclear physics; Charm (quantum number); Branching fraction; Charm quark; Standard Model (mathematical formulation); Electron–positron annihilation; Coupling (piping); Jet (fluid)","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":[],"consensus_categories":[],"category_scores_codex":[0.00009959211,0.00007477704,0.0001304859,0.00000596695,0.00003286675,0.000002941758,0.00009249523,0.000004580379,0.00004171879],"category_scores_gemma":[0.000001546732,0.0000535752,0.0000747318,0.0001562037,0.000131609,0.00004918031,0.00002790826,0.0000533304,0.00000948702],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00001584569,"about_ca_system_score_gemma":0.0000065592,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0001251619,"about_ca_topic_score_gemma":5.177023e-7,"domain_scores_codex":[0.9994473,0.00004185076,0.0001508374,0.0001073614,0.000130806,0.0001218364],"domain_scores_gemma":[0.999753,0.000007668917,0.00005458558,0.0001468619,0.00002416044,0.00001371624],"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":[0.00003328937,0.0003444929,0.02445816,0.00001257193,0.00004837216,4.874065e-8,0.0007517836,0.0005423858,0.9427401,0.01920084,0.0001242001,0.01174373],"study_design_scores_gemma":[0.000197608,0.000009519865,0.005462222,0.00003767647,0.00001071335,1.906333e-8,0.0000523962,0.00005102108,0.9773015,0.01678118,0.000037613,0.00005856276],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9967608,0.00002335485,0.0001163747,0.0009378641,0.00005091789,0.0001202274,0.000003418694,0.000003352297,0.001983694],"genre_scores_gemma":[0.9997888,0.000001246294,0.00001578144,0.00005230758,0.0001084233,0.00002010418,6.030909e-7,0.00000540935,0.000007384672],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.03456135,"threshold_uncertainty_score":0.2184733,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01741676557405687,"score_gpt":0.2327009237886039,"score_spread":0.215284158214547,"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."}}