{"id":"W4224253830","doi":"10.1103/physrevd.105.126020","title":"Melting of heavy vector mesons and quasinormal modes in a finite density plasma from holography","year":2022,"lang":"en","type":"article","venue":"Physical review. D/Physical review. D.","topic":"High-Energy Particle Collisions Research","field":"Physics and Astronomy","cited_by":0,"is_retracted":false,"has_abstract":true,"ca_institutions":"Institute of Particle Physics","funders":"Fundação Carlos Chagas Filho de Amparo à Pesquisa do Estado do Rio de Janeiro; Conselho Nacional de Desenvolvimento Científico e Tecnológico; Coordenação de Aperfeiçoamento de Pessoal de Nível Superior; National Natural Science Foundation of China","keywords":"Physics; Quantum electrodynamics; Meson; Quantum chromodynamics; Deconfinement; Quasinormal mode; Quark–gluon plasma; Perturbation theory (quantum mechanics); Dispersion relation; Long wavelength limit; Conformal map; Gravitation; 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"],"consensus_categories":[],"category_scores_codex":[0.0006601028,0.0004298365,0.001653828,0.000114329,0.0002710785,0.00003241385,0.0005655263,0.00002359077,0.0001006687],"category_scores_gemma":[0.0003135041,0.0003773354,0.0006620558,0.001612453,0.0002285105,0.000241545,0.0008047976,0.0008960776,0.00005444574],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00006222261,"about_ca_system_score_gemma":0.0001237616,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0006568118,"about_ca_topic_score_gemma":0.00001451612,"domain_scores_codex":[0.9958439,0.001052831,0.000776566,0.0007884547,0.00086105,0.0006771929],"domain_scores_gemma":[0.9969997,0.001447245,0.0003329847,0.0007630053,0.0001339283,0.0003230762],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"observational","study_design_gemma":"simulation_or_modeling","study_design_scores_codex":[0.0005110127,0.01359857,0.3692989,0.00711304,0.001017228,0.0001063114,0.001592553,0.005857798,0.137198,0.3612423,0.003375686,0.09908862],"study_design_scores_gemma":[0.006804639,0.002713725,0.1594926,0.02371852,0.002635026,0.00001340871,0.0007397069,0.6173044,0.07502627,0.06820931,0.03825055,0.005091828],"study_design_candidate":"simulation_or_modeling","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9867002,0.01063103,0.0000674806,0.0007112458,0.00003775479,0.0008717857,0.0002413494,0.00003279819,0.000706397],"genre_scores_gemma":[0.9935071,0.005162232,0.000274916,0.0001545372,0.0002207642,0.0005302254,0.00009339,0.00004359588,0.00001318994],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.6114466,"threshold_uncertainty_score":0.9998679,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02044551879236808,"score_gpt":0.4034865288520249,"score_spread":0.3830410100596568,"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."}}