{"id":"W2321906901","doi":"10.1103/physrevlett.87.052301","title":"Measurement of the Midrapidity Transverse Energy Distribution from<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msqrt><mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mi>NN</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:msqrt><mml:mspace/><mml:mo>=</mml:mo><mml:mspace/><mml:mn>130</mml:mn><mml:mn/><mml:mi/><mml:mi>GeV</mml:mi></mml:math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>A</mml:mi><mml:mi>u</mml:mi><mml:mo>+</mml:mo><mml:mi>A</mml:mi><mml:mi>u</mml:mi></mml:math>Collisions at RHIC","year":2001,"lang":"lv","type":"article","venue":"Physical Review Letters","topic":"High-Energy Particle Collisions Research","field":"Physics and Astronomy","cited_by":148,"is_retracted":false,"has_abstract":true,"ca_institutions":"McGill University","funders":"","keywords":"Physics; Nuclear physics; Large Hadron Collider; Transverse plane; National laboratory; Nucleon; Relativistic Heavy Ion Collider; Energy (signal processing); Collider; Particle physics; Heavy ion; Ion; Engineering physics; Quantum mechanics","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":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0007609925,0.0006696369,0.0003523818,0.001418781,0.001051427,0.001386397,0.0008558469,0.0009342569,0.04736024],"category_scores_gemma":[0.0007895984,0.0006564364,0.0005799715,0.001275909,0.0002414051,0.0008862346,0.001021913,0.001301129,0.02221666],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.001069361,"about_ca_system_score_gemma":0.0007906115,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.005450381,"about_ca_topic_score_gemma":0.008109311,"domain_scores_codex":[0.9994992,0.00004161453,0.00001497237,0.0001147887,0.0002375607,0.00009178883],"domain_scores_gemma":[0.9995545,0.00006727222,0.00005119372,0.00007599829,0.000175993,0.00007498397],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"bench_or_experimental","study_design_gemma":"observational","study_design_scores_codex":[0.003135446,0.0003926565,0.03036628,0.0005332144,0.0002544672,0.001336639,0.0006438244,0.003048517,0.5977725,0.02600581,0.2205726,0.1159381],"study_design_scores_gemma":[0.0002580715,0.0005355372,0.125477,0.0001536209,0.0001104321,0.001375688,0.0003438612,0.02816064,0.6213387,0.005300767,0.2167004,0.0002453575],"study_design_candidate":"observational","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.3700834,0.001797268,0.1435379,0.003114898,0.0009450232,0.0003389234,0.0921353,0.02169375,0.3663535],"genre_scores_gemma":[0.7209341,0.001103754,0.06084232,0.001327602,0.0001472055,0.0004084544,0.07166198,0.006214982,0.1373597],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.04736024,"threshold_uncertainty_score":0.1584358,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02215407864517162,"score_gpt":0.2553705314365204,"score_spread":0.2332164527913488,"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."}}