{"id":"W2068742253","doi":"10.1016/j.nuclphysa.2014.08.078","title":"Probing the non-equilibrium dynamics of hot and dense QCD with dileptons","year":2014,"lang":"en","type":"article","venue":"Nuclear Physics A","topic":"High-Energy Particle Collisions Research","field":"Physics and Astronomy","cited_by":7,"is_retracted":false,"has_abstract":false,"ca_institutions":"McGill University","funders":"Nuclear Physics; U.S. Department of Energy; Fonds Québécois de la Recherche sur la Nature et les Technologies; Natural Sciences and Engineering Research Council of Canada; Government of Canada; Canada Foundation for Innovation","keywords":"Physics; Hadron; Observable; Anisotropy; Nuclear physics; Thermal diffusivity; Cauchy stress tensor; Viscosity; Relaxation (psychology); Thermal; Classical mechanics; Thermodynamics; Optics; Quantum mechanics","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":[0.001294305,0.0004763987,0.0005355342,0.0006729288,0.0008309049,0.001822124,0.001175674,0.000492332,0.004975863],"category_scores_gemma":[0.003345657,0.0007437401,0.0002770128,0.0008431869,0.00221581,0.002216724,0.002004714,0.001476898,0.0003345269],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00135942,"about_ca_system_score_gemma":0.0005060609,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.00160598,"about_ca_topic_score_gemma":0.00173181,"domain_scores_codex":[0.9994911,0.000101509,0.00001322509,0.0001225588,0.0001024698,0.0001691152],"domain_scores_gemma":[0.9981329,0.001020982,0.0002835632,0.0001694009,0.00009546237,0.0002977905],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"simulation_or_modeling","study_design_scores_codex":[0.004923418,0.002058471,0.09674457,0.0007162796,0.0005361096,0.002414806,0.003361301,0.1512062,0.3341475,0.3599229,0.005368686,0.03859978],"study_design_scores_gemma":[0.0009149872,0.0007083032,0.0445567,0.00007719015,0.0001341376,0.0008504028,0.001466918,0.6452322,0.1213018,0.180176,0.004318635,0.0002627945],"study_design_candidate":"simulation_or_modeling","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9763203,0.0003278305,0.01137588,0.0003517998,0.00005274361,0.00002917029,0.000226381,0.0002394092,0.01107661],"genre_scores_gemma":[0.9978166,0.00005088528,0.001351895,0.00006446904,0.00001213473,0.000008071101,0.00006083147,0.00002927543,0.0006058083],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.004975863,"threshold_uncertainty_score":0.01664591,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.007581694969358411,"score_gpt":0.2289319101840458,"score_spread":0.2213502152146874,"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."}}