{"id":"W2743658653","doi":"10.1103/physrevlett.94.171802","title":"Measurement of Charged-Particle Multiplicities in Gluon and Quark Jets in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>p</mml:mi><mml:mover accent=\"true\"><mml:mi>p</mml:mi><mml:mo>¯</mml:mo></mml:mover></mml:math>Collisions at<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msqrt><mml:mi>s</mml:mi></mml:msqrt><mml:mo>=</mml:mo><mml:mn>1.8</mml:mn><mml:mtext>   </mml:mtext><mml:mi>TeV</mml:mi></mml:math>","year":2005,"lang":"lv","type":"article","venue":"Physical Review Letters","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":16,"is_retracted":false,"has_abstract":true,"ca_institutions":"Institute of Particle Physics; University of Toronto","funders":"Natural Sciences and Engineering Research Council of Canada; Istituto Nazionale di Fisica Nucleare; National Science Council; Alfred P. Sloan Foundation; Fermilab; U.S. Department of Energy; Ministry of Education, Culture, Sports, Science and Technology; National Science Foundation","keywords":"Physics; Particle physics; Gluon; Collider Detector at Fermilab; Tevatron; Quantum chromodynamics; Top quark; Fermilab; Nuclear physics; Standard Model (mathematical formulation); Collider; Jet (fluid); Perturbative QCD; Quark; Large Hadron Collider; Gauge (firearms)","routes":{"ca_aff":true,"ca_fund":true,"ca_venue":false,"about_ca":false,"invisible_to_affiliation_only":false},"retraction":null,"screen":null,"direct_labels":[],"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0006079861,0.0007015971,0.0004593974,0.001111268,0.0007687957,0.001025681,0.0009142887,0.0008212012,0.004137075],"category_scores_gemma":[0.001167818,0.0004911183,0.0003869101,0.001003727,0.000421288,0.000773922,0.0008619353,0.0006217586,0.0007240011],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0009129586,"about_ca_system_score_gemma":0.0002992672,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.003603485,"about_ca_topic_score_gemma":0.008067321,"domain_scores_codex":[0.9994462,0.00007884914,0.00001992493,0.0001616047,0.0002230566,0.00007041484],"domain_scores_gemma":[0.9993319,0.0002224563,0.0001493598,0.0001295614,0.00009548338,0.00007110138],"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":[0.002402783,0.0003591505,0.1460973,0.0003073709,0.0003198322,0.002060789,0.001097585,0.00433683,0.8092235,0.004482406,0.004586876,0.02472553],"study_design_scores_gemma":[0.0001579995,0.00100456,0.1973221,0.00003485903,0.0001714915,0.001528661,0.0002967318,0.02079358,0.7642868,0.00185702,0.01238815,0.0001581503],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9656612,0.0004860071,0.01760325,0.0001645156,0.00005883431,0.0000792834,0.004363339,0.0009048618,0.01067874],"genre_scores_gemma":[0.9875359,0.00017341,0.005673048,0.00006432922,0.00001504845,0.00003872058,0.002565956,0.00009473609,0.003838867],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.004137075,"threshold_uncertainty_score":0.0138399,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02075556149623403,"score_gpt":0.2607767045856966,"score_spread":0.2400211430894626,"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."}}