{"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":"codex-gemma-dda1882f352a","candidate_categories":["metaepi_narrow","metaepi_broad","sts","scholarly_communication","open_science","research_integrity","insufficient_payload"],"consensus_categories":["metaepi_narrow","sts","open_science","research_integrity","insufficient_payload"],"category_scores_codex":[0.007717261,0.004104237,0.001724479,0.002049996,0.007596555,0.005454764,0.009972545,0.006901562,0.5253479],"category_scores_gemma":[0.006299955,0.007893111,0.01026637,0.006497297,0.007941282,0.005623406,0.008611644,0.007704949,0.008208279],"about_ca_system_candidate":true,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0001465154,"about_ca_system_score_gemma":0.006978787,"about_ca_topic_candidate":true,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.009821238,"about_ca_topic_score_gemma":0.008233928,"domain_scores_codex":[0.9602754,0.003186027,0.007544568,0.007380041,0.01165408,0.009959889],"domain_scores_gemma":[0.9690557,0.006341566,0.008478904,0.009411936,0.001106868,0.005605038],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.004504671,0.001811318,0.00004704217,0.003755328,0.006545891,0.00341348,0.002578208,0.007973765,0.009604767,0.4797674,0.4766743,0.003323732],"study_design_scores_gemma":[0.006573798,0.004582604,0.000209139,0.007467453,0.008378482,0.002842184,0.00366381,0.04247967,0.8915223,0.0007242252,0.02478753,0.006768731],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.6314242,0.006893322,0.00352273,0.00478349,0.008066898,0.000266475,0.00349493,0.0009645044,0.3405834],"genre_scores_gemma":[0.952852,0.009840136,0.003130488,0.004684131,0.008245034,0.008021786,0.00894644,0.003708079,0.0005718992],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.8819176,"threshold_uncertainty_score":0.9996456,"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."}}