{"id":"W4308588150","doi":"10.1016/j.nds.2022.10.002","title":"Nuclear Structure and Decay Data for A=231 Isobars","year":2022,"lang":"en","type":"article","venue":"Nuclear Data Sheets","topic":"Nuclear physics research studies","field":"Physics and Astronomy","cited_by":6,"is_retracted":false,"has_abstract":false,"ca_institutions":"McMaster University","funders":"Brookhaven National Laboratory","keywords":"Excited state; Nuclide; Isobar; Physics; Atomic physics; Spins; Nuclear structure; Coulomb excitation; Excitation; Nuclear physics; Spin (aerodynamics); Nuclear data; Branching fraction; Nucleon; Neutron","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":["open_science","insufficient_payload"],"consensus_categories":[],"category_scores_codex":[0.0002971118,0.0002116254,0.0002668763,0.00005968228,0.00103317,0.0002033176,0.002498637,0.00002540819,0.004979144],"category_scores_gemma":[0.00002469584,0.0002160094,0.00003926926,0.0001701945,0.0001384039,0.0006805511,0.01063194,0.0003983456,0.0000577888],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00002998081,"about_ca_system_score_gemma":0.00004573999,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.000143623,"about_ca_topic_score_gemma":0.000004501848,"domain_scores_codex":[0.9979932,0.00007697718,0.0001982262,0.0008748643,0.0003988437,0.0004578608],"domain_scores_gemma":[0.9970936,0.00009842117,0.00008990279,0.00253509,0.0000454968,0.0001375139],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"not_applicable","study_design_gemma":"not_applicable","study_design_scores_codex":[0.0001371833,0.0001973267,0.0006546704,0.0000552976,0.0004233176,0.000005020629,0.0007031948,0.00002763618,0.003679345,0.04194861,0.8777837,0.07438473],"study_design_scores_gemma":[0.0007835275,0.00009787529,0.0008618943,0.000007175383,0.00005571326,0.000003113091,0.00172306,0.01192324,0.00002198315,0.002242477,0.9819739,0.0003059701],"study_design_candidate":"not_applicable","study_design_consensus":"not_applicable","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.68828,0.0007413237,0.000382599,0.007357712,0.001116449,0.00367619,0.2579713,0.0005307562,0.03994361],"genre_scores_gemma":[0.9912319,0.00001543832,0.002273845,0.000267559,0.0004314297,0.0000112261,0.005441668,0.0001251443,0.0002017947],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.3029518,"threshold_uncertainty_score":0.9973699,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.04868196986293261,"score_gpt":0.3154518917512728,"score_spread":0.2667699218883401,"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."}}