{"id":"W4221161170","doi":"10.1103/physrevc.106.064901","title":"Role of bulk viscosity in deuteron production in ultrarelativistic nuclear collisions","year":2022,"lang":"en","type":"article","venue":"Physical review. C","topic":"High-Energy Particle Collisions Research","field":"Physics and Astronomy","cited_by":14,"is_retracted":false,"has_abstract":true,"ca_institutions":"McGill University; University of Regina","funders":"Natural Sciences and Engineering Research Council of Canada; Office of Science; Nuclear Physics; Central China Normal University; National Natural Science Foundation of China; University of Texas at Austin; Alexander von Humboldt-Stiftung; Fundação de Amparo à Pesquisa do Estado de São Paulo; U.S. Department of Energy; Wayne State University; National Science Foundation","keywords":"Physics; Deuterium; Nuclear physics; Large Hadron Collider; Coalescence (physics); Hadron; Elliptic flow; Observable; Particle physics; Heavy ion","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":"codex-gemma-dda1882f352a","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0003157147,0.000100067,0.000312054,0.00008086571,0.0001017304,0.000008285312,0.0002070361,0.000007765919,0.0002104419],"category_scores_gemma":[0.00008268467,0.00009537958,0.00008867799,0.0009745701,0.00004616949,0.0001088056,0.000183299,0.0003443153,0.00004489848],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00008926684,"about_ca_system_score_gemma":0.00005501036,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0002310049,"about_ca_topic_score_gemma":0.000007364851,"domain_scores_codex":[0.9986036,0.0002987439,0.0002805189,0.000267622,0.0003233399,0.0002261212],"domain_scores_gemma":[0.9994063,0.0001194169,0.00007650434,0.0003001948,0.00003773006,0.0000598363],"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":[0.0002581678,0.01308197,0.1687858,0.0006394651,0.00011409,0.00001709338,0.003702007,0.1874561,0.1925411,0.3943501,0.00175525,0.03729886],"study_design_scores_gemma":[0.00377013,0.001473067,0.3890533,0.003853702,0.0002060574,0.000006613694,0.002001535,0.4518013,0.03134654,0.06166979,0.05293747,0.001880515],"study_design_candidate":"simulation_or_modeling","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9968264,0.0003582707,0.00001650296,0.0002411499,0.00002952727,0.0004230716,0.00002277622,0.000008745564,0.002073591],"genre_scores_gemma":[0.9995355,0.00007602735,0.00005422699,0.000007108525,0.00005703249,0.0001615667,0.00001574332,0.00001412147,0.00007866862],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.3326803,"threshold_uncertainty_score":0.3889466,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01411839614837939,"score_gpt":0.3196983108654365,"score_spread":0.3055799147170571,"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."}}