{"id":"W4282832843","doi":"10.1093/mnras/stac1603","title":"Hot-mode accretion and the physics of thin-disc galaxy formation","year":2022,"lang":"en","type":"article","venue":"Monthly Notices of the Royal Astronomical Society","topic":"Galaxies: Formation, Evolution, Phenomena","field":"Physics and Astronomy","cited_by":90,"is_retracted":false,"has_abstract":true,"ca_institutions":"","funders":"Science and Technology Facilities Council; University of California, Irvine; Kavli Institute for Theoretical Physics, University of California, Santa Barbara; Higher Education Commission, Pakistan; Israel Science Foundation; Flatiron Health; Pomona College; Space Telescope Science Institute; Northwestern University; Simons Foundation; Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung; Steele Foundation; California Institute of Technology; National Aeronautics and Space Administration; Nuclear Safety and Security Commission; Heising-Simons Foundation; Research Corporation for Science Advancement; Petroleum Research Newfoundland and Labrador; National Science Foundation","keywords":"Physics; Astrophysics; Thin disk; Galaxy; Accretion (finance); Thick disk; Cooling flow; Angular momentum; Halo; Radiative cooling; Galaxy formation and evolution; Astronomy; Disc galaxy; Solar mass; Stellar mass; Dark matter halo; Star formation","routes":{"ca_aff":false,"ca_fund":true,"ca_venue":false,"about_ca":false,"invisible_to_affiliation_only":true},"retraction":null,"screen":null,"direct_labels":[],"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0005167331,0.0002853345,0.0003433457,0.0005320203,0.0004208877,0.001023813,0.0008870693,0.000564343,0.001002849],"category_scores_gemma":[0.00268631,0.0002657054,0.0004081604,0.0003098247,0.000758241,0.0006493853,0.0004943174,0.0003083401,0.0001244507],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.000956355,"about_ca_system_score_gemma":0.0003984038,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.01673767,"about_ca_topic_score_gemma":0.007818888,"domain_scores_codex":[0.9999198,0.00002705243,0.000003804647,0.00001266932,0.00001163778,0.00002499575],"domain_scores_gemma":[0.9991523,0.0003883322,0.0001980876,0.00006841755,0.00005788067,0.0001349965],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"simulation_or_modeling","study_design_gemma":"simulation_or_modeling","study_design_scores_codex":[0.000251947,0.0001270047,0.2166281,0.00003767393,0.0001255198,0.0004265505,0.0002664283,0.7661626,0.005318302,0.007461036,0.0002930526,0.002901905],"study_design_scores_gemma":[0.00006521301,0.00005634369,0.03853326,0.000009263021,0.00002073559,0.00006977743,0.0000919393,0.9569408,0.001248167,0.002688529,0.0002615822,0.00001443018],"study_design_candidate":"simulation_or_modeling","study_design_consensus":"simulation_or_modeling","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9981301,0.00003973066,0.0008750072,0.0000396859,0.000002477003,0.000004832133,0.0000662348,0.00001969547,0.0008220826],"genre_scores_gemma":[0.9994099,0.00002777185,0.000345328,0.000009798209,0.000002021001,0.000003282008,0.00004628516,0.00000493155,0.0001507638],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.01673767,"threshold_uncertainty_score":0.03328049,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.005984716520160276,"score_gpt":0.1952101075209343,"score_spread":0.1892253910007741,"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."}}