{"id":"W7071945177","doi":"","title":"Top quark mass measurement in the t(t)over bar all hadronic channel using a matrix element technique in p(p)over bar collisions at root s=1.96 TeV","year":2009,"lang":"en","type":"article","venue":"Purdue e-Pubs (Purdue University System)","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":0,"is_retracted":false,"has_abstract":true,"ca_institutions":"","funders":"Fermilab; Science and Technology Facilities Council; Alfred P. Sloan Foundation; National Science Council; Natural Sciences and Engineering Research Council of Canada; Istituto Nazionale di Fisica Nucleare; Centre National de la Recherche Scientifique; U.S. Department of Energy; Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung; Russian Foundation for Basic Research; Ministry of Education, Culture, Sports, Science and Technology; National Science Foundation","keywords":"Top quark; Hadron; Invariant mass; Fermilab; Tevatron; Bar (unit); Jet (fluid); Quark; Bottom quark","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":[0.0007739711,0.0005389299,0.0003146869,0.0009828723,0.0004065551,0.001076711,0.0006774347,0.0004861696,0.002154257],"category_scores_gemma":[0.001642786,0.0004078557,0.0005422558,0.001131466,0.0002965814,0.0005349837,0.0005210857,0.00031423,0.0003925283],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0004657886,"about_ca_system_score_gemma":0.0002295855,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.001904258,"about_ca_topic_score_gemma":0.002850679,"domain_scores_codex":[0.9994816,0.00008492622,0.00001982155,0.0001843459,0.0001650285,0.00006437714],"domain_scores_gemma":[0.9988148,0.0004037459,0.0003638203,0.0001723447,0.0001356478,0.0001095846],"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":[0.004310174,0.0003675594,0.5431744,0.0001904556,0.0004375207,0.001326285,0.0003818898,0.03560331,0.3624321,0.005400561,0.001046934,0.04532867],"study_design_scores_gemma":[0.0001689304,0.001315023,0.4093353,0.00002665455,0.0004222804,0.002744195,0.0001607713,0.1451638,0.434366,0.003729637,0.002405885,0.0001615781],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9818194,0.00008626851,0.01469632,0.00002616311,0.000008219048,0.00002219638,0.001065427,0.0003067174,0.001969374],"genre_scores_gemma":[0.9937288,0.0000405302,0.005181962,0.00001195646,0.000005227568,0.00001347399,0.0005757277,0.00002709148,0.0004151635],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.002154257,"threshold_uncertainty_score":0.007206738,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01772041419533394,"score_gpt":0.2464143414970723,"score_spread":0.2286939273017383,"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."}}