{"id":"W2901152217","doi":"10.1103/physrevc.98.054307","title":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mi>β</mml:mi></mml:math>-decay half-lives of <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi>Sb</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>134</mml:mn><mml:mo>,</mml:mo><mml:mn>134</mml:mn><mml:mi>m</mml:mi></mml:mrow></mml:mmultiscripts></mml:math> and their isomeric yield ratio produced by the spontaneous fission of <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi>Cf</mml:mi><mml:mprescripts/><mml:none/><mml:mn>252</mml:mn></mml:mmultiscripts></mml:math>","year":2018,"lang":"lv","type":"article","venue":"Physical review. C","topic":"Nuclear physics research studies","field":"Physics and Astronomy","cited_by":8,"is_retracted":false,"has_abstract":true,"ca_institutions":"","funders":"Lawrence Livermore National Laboratory; Nuclear Physics; Australian Research Council; Nuclear Safety and Security Commission; University of Notre Dame; U.S. Department of Energy; Natural Sciences and Engineering Research Council of Canada; National Nuclear Security Administration; National Science Foundation","keywords":"Physics; Spontaneous fission; Fission; Yield (engineering); Fission product yield; Atomic physics; Ground state; Nuclear physics; Energy (signal processing); Neutron","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":"codex-gemma-dda1882f352a","candidate_categories":["metaepi_narrow","sts","scholarly_communication","open_science","research_integrity","insufficient_payload"],"consensus_categories":["metaepi_narrow","sts","open_science","research_integrity","insufficient_payload"],"category_scores_codex":[0.006640703,0.004708458,0.002550809,0.001645265,0.007178117,0.004931561,0.009188405,0.005424437,0.03966805],"category_scores_gemma":[0.005727486,0.007226347,0.007857355,0.004349464,0.008782375,0.005805877,0.01007227,0.007733009,0.007682863],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0001430164,"about_ca_system_score_gemma":0.004707913,"about_ca_topic_candidate":true,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.008103546,"about_ca_topic_score_gemma":0.002513975,"domain_scores_codex":[0.9651022,0.002544447,0.007648306,0.007393809,0.008665317,0.008645952],"domain_scores_gemma":[0.9707021,0.00554954,0.009009995,0.009406151,0.001347485,0.003984748],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.004155669,0.002512614,0.00002139052,0.005951268,0.006795156,0.002206781,0.007483081,0.001006436,0.03114036,0.7246928,0.2057853,0.008249104],"study_design_scores_gemma":[0.005815956,0.006332228,0.000107229,0.008564442,0.006325495,0.002878917,0.007584284,0.1753802,0.74745,0.001566552,0.03173587,0.006258785],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.8646001,0.01207704,0.001492101,0.002066375,0.008108663,0.000616595,0.003900767,0.001162023,0.1059764],"genre_scores_gemma":[0.957826,0.0118997,0.004043944,0.003216086,0.007070655,0.006318705,0.005208171,0.003469345,0.0009474009],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.7231263,"threshold_uncertainty_score":0.9985016,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02436104260974747,"score_gpt":0.2648872805173645,"score_spread":0.2405262379076171,"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."}}