{"id":"W2749131085","doi":"10.1103/physrevc.96.024305","title":"Doppler-shift attenuation lifetime measurement of the <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi mathvariant=\"bold\">Ar</mml:mi><mml:mprescripts/><mml:none/><mml:mn>36</mml:mn></mml:mmultiscripts><mml:mspace width=\"4.pt\"/><mml:msubsup><mml:mn>2</mml:mn><mml:mn>1</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:math> level","year":2017,"lang":"lv","type":"article","venue":"Physical review. C","topic":"Nuclear physics research studies","field":"Physics and Astronomy","cited_by":3,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of British Columbia; TRIUMF; University of Toronto; University of Guelph; Simon Fraser University","funders":"National Research Council Canada; Natural Sciences and Engineering Research Council of Canada; Simon Fraser University; TRIUMF","keywords":"Physics; Coulomb excitation; Atomic physics; Energy (signal processing); Excited state; Quadrupole; Doppler effect; Excitation","routes":{"ca_aff":true,"ca_fund":true,"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":[0.0006663202,0.0004983085,0.0003872739,0.0008806839,0.0005401488,0.0006020797,0.0009404052,0.0006567079,0.0139793],"category_scores_gemma":[0.000961397,0.000292069,0.0002473232,0.0007726364,0.0002892436,0.0007131633,0.000529562,0.0009151092,0.002543969],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0008160597,"about_ca_system_score_gemma":0.0007237745,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.002608646,"about_ca_topic_score_gemma":0.003549744,"domain_scores_codex":[0.999724,0.00002145278,0.000007862184,0.0001086093,0.00007771747,0.00006034211],"domain_scores_gemma":[0.999524,0.00009942786,0.00006769802,0.00009279521,0.0001768259,0.00003929099],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"bench_or_experimental","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.0005681057,0.0001274457,0.003382848,0.0001102606,0.00002787364,0.0001071832,0.0002943259,0.0007438041,0.9691826,0.002147667,0.003345022,0.01996286],"study_design_scores_gemma":[0.00001014812,0.0001682714,0.003904653,0.00000783543,0.00001864945,0.00008954766,0.00004559919,0.003712623,0.9835808,0.0001511394,0.008289372,0.00002124965],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.8310503,0.001083563,0.1227032,0.0004486725,0.0001847574,0.0001614529,0.005542617,0.006389395,0.03243609],"genre_scores_gemma":[0.9238548,0.0005424319,0.04640443,0.0001456319,0.00001952843,0.0001704998,0.003391451,0.001060176,0.0244111],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.0139793,"threshold_uncertainty_score":0.04676539,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.0434620213708926,"score_gpt":0.2879065282994627,"score_spread":0.2444445069285701,"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."}}