{"id":"W4319927086","doi":"10.1103/physrevlett.130.062501","title":"Final Result of the Majorana Demonstrator’s Search for Neutrinoless Double-<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>β</mml:mi></mml:math> Decay in <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi>Ge</mml:mi></mml:mrow><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>76</mml:mn></mml:mrow></mml:mmultiscripts></mml:mrow></mml:math>","year":2023,"lang":"lv","type":"article","venue":"Physical Review Letters","topic":"Neutrino Physics Research","field":"Physics and Astronomy","cited_by":85,"is_retracted":false,"has_abstract":true,"ca_institutions":"Queen's University","funders":"Los Alamos National Laboratory; Lawrence Berkeley National Laboratory; Oak Ridge National Laboratory; Laboratory Directed Research and Development; Nuclear Physics; Natural Sciences and Engineering Research Council of Canada; Jet Propulsion Laboratory; Pacific Northwest National Laboratory; National Energy Research Scientific Computing Center; Universität Hamburg; Canada Foundation for Innovation; SLAC National Accelerator Laboratory; Division of Physics; South Dakota Board of Regents; Office of Science; California Institute of Technology; U.S. Department of Energy; National Science Foundation","keywords":"MAJORANA; Physics; Double beta decay; Particle physics; Nuclear physics; Neutrino","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":[0.001955787,0.001198994,0.0008435465,0.0006023449,0.00153087,0.00131744,0.001182271,0.001609352,0.01869399],"category_scores_gemma":[0.001031731,0.0006214129,0.001065706,0.0005248027,0.000447491,0.0008757047,0.001539018,0.001082461,0.01225332],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0008253232,"about_ca_system_score_gemma":0.0008087399,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0017296,"about_ca_topic_score_gemma":0.002820484,"domain_scores_codex":[0.9991098,0.00008936977,0.00002390037,0.0002632685,0.0003216261,0.0001920349],"domain_scores_gemma":[0.9984825,0.0001893076,0.00009873523,0.0002759418,0.00056787,0.0003855145],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"bench_or_experimental","study_design_gemma":"observational","study_design_scores_codex":[0.008388402,0.001167484,0.03712947,0.0008288551,0.0005788455,0.00750474,0.001734495,0.003074385,0.6759261,0.006272918,0.1540786,0.1033157],"study_design_scores_gemma":[0.0007089388,0.003510812,0.05384306,0.00005715734,0.000360266,0.004931746,0.0007576686,0.009307576,0.7248348,0.002304978,0.1991182,0.0002648484],"study_design_candidate":"observational","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.7551883,0.0008363337,0.06165304,0.004744504,0.0008763398,0.0008856186,0.02809543,0.01421301,0.1335075],"genre_scores_gemma":[0.7590768,0.0002449341,0.08381307,0.001329564,0.0002263331,0.0003762426,0.04097198,0.00436824,0.109593],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.01869399,"threshold_uncertainty_score":0.06253761,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.03571784989178849,"score_gpt":0.2873865728149696,"score_spread":0.2516687229231811,"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."}}