{"id":"W4306352951","doi":"10.1093/mnras/stac2951","title":"Testing afterglow models of FRB 200428 with early post-burst observations of SGR 1935 + 2154","year":2022,"lang":"en","type":"article","venue":"Monthly Notices of the Royal Astronomical Society","topic":"Pulsars and Gravitational Waves Research","field":"Physics and Astronomy","cited_by":9,"is_retracted":false,"has_abstract":true,"ca_institutions":"Canadian Institute for Theoretical Astrophysics; University of Toronto","funders":"Science and Technology Facilities Council; College of Natural Resources and Sciences, Humboldt State University; Ministerium für Innovation, Wissenschaft und Forschung des Landes Nordrhein-Westfalen; Max-Planck-Gesellschaft; Ministerstwo Edukacji i Nauki; Nederlandse Organisatie voor Wetenschappelijk Onderzoek; Bundesministerium für Bildung und Forschung; Science Foundation Ireland; Department of Jobs, Enterprise and Innovation","keywords":"Physics; Afterglow; Magnetar; Astrophysics; Fast radio burst; Maser; Astronomy; LOFAR; Luminosity; Radio telescope; Gamma-ray burst; Very-long-baseline interferometry; Pulsar; Neutron star; Galaxy","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":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.002751958,0.000545153,0.0004592201,0.0006412706,0.0005773052,0.001379009,0.001271148,0.0006156279,0.00236472],"category_scores_gemma":[0.004558047,0.0003278227,0.0008556846,0.000350186,0.0006618343,0.0007386176,0.0007822236,0.0004218853,0.000435605],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.001536954,"about_ca_system_score_gemma":0.000464731,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.02271124,"about_ca_topic_score_gemma":0.01618427,"domain_scores_codex":[0.9994074,0.0002034603,0.0000349849,0.0001616885,0.00007522864,0.0001171846],"domain_scores_gemma":[0.9956671,0.001918564,0.000985542,0.0004695536,0.0003209249,0.0006382592],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"observational","study_design_gemma":"observational","study_design_scores_codex":[0.0009664346,0.0001777247,0.9680472,0.00003479821,0.0002615362,0.000368111,0.0002991987,0.01345932,0.009187089,0.0009844687,0.0003838178,0.005830242],"study_design_scores_gemma":[0.0001143604,0.000584582,0.9140872,0.0000213904,0.0001136967,0.0001464642,0.000488636,0.08098093,0.002126358,0.0006999648,0.0006059441,0.00003048673],"study_design_candidate":"observational","study_design_consensus":"observational","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9981816,0.00003352611,0.0006935251,0.00007742237,0.000005283301,0.00000938734,0.0001080931,0.00003363644,0.0008576294],"genre_scores_gemma":[0.9994572,0.00001089653,0.000249736,0.00001713124,0.000005055001,0.000004458802,0.0001772419,0.000008565207,0.00006964265],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.02271124,"threshold_uncertainty_score":0.04515809,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01938404673060567,"score_gpt":0.2455275923895066,"score_spread":0.2261435456589009,"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."}}