{"id":"W1559954614","doi":"10.2172/842927","title":"Qcd physics: study of jet shapes in inclusive jet production in ppbar collisions at sqrt s = 1.96 tev","year":2005,"lang":"en","type":"report","venue":"","topic":"High-Energy Particle Collisions Research","field":"Physics and Astronomy","cited_by":0,"is_retracted":false,"has_abstract":true,"ca_institutions":"","funders":"Natural Sciences and Engineering Research Council of Canada; Istituto Nazionale di Fisica Nucleare; Bundesministerium für Bildung und Forschung; National Science Council; Alfred P. Sloan Foundation; Fermilab; 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":"Physics; Particle physics; Lambda; Excited state; Production (economics); Nuclear physics; Quantum chromodynamics; Electron; Jet (fluid); Standard Model (mathematical formulation); Coupling (piping); Gauge (firearms)","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":[0.0007252663,0.0004508411,0.0003476287,0.00115027,0.0003921576,0.0007111998,0.0006413012,0.0003812656,0.00153608],"category_scores_gemma":[0.002564715,0.000388028,0.0003374728,0.001564232,0.0003835698,0.000336265,0.0004124284,0.0004163609,0.0004200203],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0006578167,"about_ca_system_score_gemma":0.0002400413,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0009271155,"about_ca_topic_score_gemma":0.0006873829,"domain_scores_codex":[0.9996756,0.0001132944,0.00001214376,0.00006926795,0.00009491773,0.00003484749],"domain_scores_gemma":[0.9985197,0.0008058209,0.0003316251,0.00008267603,0.0001140415,0.0001461409],"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":[0.00644773,0.0008111685,0.4917053,0.000815261,0.0004975912,0.007330761,0.0009926615,0.1434358,0.2668839,0.02033937,0.00373764,0.05700289],"study_design_scores_gemma":[0.000336385,0.0009106344,0.4129415,0.00003512644,0.0001147807,0.006008144,0.000271908,0.4515029,0.1142267,0.01048824,0.00300531,0.0001584778],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9917797,0.0002256809,0.004431602,0.00006348926,0.000006992973,0.00001565555,0.0007370086,0.0002171377,0.002522671],"genre_scores_gemma":[0.9967353,0.00006994019,0.001986252,0.00001461615,0.000007853555,0.00001133233,0.0005743737,0.00005974866,0.0005406123],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.00153608,"threshold_uncertainty_score":0.005138695,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.03727782547573074,"score_gpt":0.3539729798990818,"score_spread":0.3166951544233511,"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."}}