{"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":"codex-gemma-dda1882f352a","candidate_categories":["metaepi_narrow","insufficient_payload"],"consensus_categories":[],"category_scores_codex":[0.001045472,0.0005101825,0.001084292,0.0006357323,0.0002025812,0.00005041286,0.0004515961,0.0001951913,0.001104848],"category_scores_gemma":[0.0001673427,0.0004303836,0.0001898909,0.001693476,0.000110625,0.0002801087,0.001075532,0.000785405,0.0001207674],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.001040303,"about_ca_system_score_gemma":0.001445275,"about_ca_topic_candidate":true,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.01572181,"about_ca_topic_score_gemma":0.00804738,"domain_scores_codex":[0.9951645,0.000342326,0.001214565,0.001019392,0.001604807,0.0006543978],"domain_scores_gemma":[0.9976187,0.0001845395,0.0004023594,0.0008692103,0.0007683699,0.0001567601],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"observational","study_design_gemma":"observational","study_design_scores_codex":[0.000146431,0.009818057,0.8551211,0.0001023139,0.0003752615,0.00005649839,0.002848788,0.1122457,0.002177754,0.001095566,0.007968896,0.008043648],"study_design_scores_gemma":[0.02035924,0.004124715,0.5211193,0.003924361,0.000890721,0.00003742829,0.04171629,0.06383193,0.1223284,0.001202876,0.2128028,0.007661942],"study_design_candidate":"observational","study_design_consensus":"observational","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9655968,0.0000867405,0.00002731695,0.0001526186,0.0002211399,0.001919768,0.0001095136,0.00003081128,0.03185532],"genre_scores_gemma":[0.9879544,0.00009087822,0.0001643103,0.00000157585,0.001037122,0.0005789654,0.000152099,0.00007651973,0.009944152],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.3340018,"threshold_uncertainty_score":0.9998148,"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."}}