{"id":"W3204358447","doi":"10.1088/1361-6471/ac2b0f","title":"The status and future of direct nuclear reaction measurements for stellar burning","year":2021,"lang":"en","type":"article","venue":"Journal of Physics G Nuclear and Particle Physics","topic":"Stellar, planetary, and galactic studies","field":"Physics and Astronomy","cited_by":24,"is_retracted":false,"has_abstract":true,"ca_institutions":"TRIUMF","funders":"ExtreMe Matter Institute, GSI Helmholtzzentrum für Schwerionenforschung; European Cooperation in Science and Technology; Office of International Science and Engineering; Institutul de Fizică Atomică; Emberi Eroforrások Minisztériuma; Los Alamos National Laboratory; Joint Institute for Nuclear Astrophysics - Center for the Evolution of the Elements; National Nuclear Security Administration; U.S. Department of Energy; European Commission; Laboratory Directed Research and Development; National Science Foundation","keywords":"Nucleosynthesis; Prospectus; Stellar nucleosynthesis; Stellar evolution; Physics; Nuclear astrophysics; Stellar physics; Stars; Astronomy; Stellar collision; Stellar atmosphere","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":[0.01552114,0.001607559,0.002453728,0.002511884,0.0008745827,0.003692262,0.002952438,0.002798258,0.007916993],"category_scores_gemma":[0.01143376,0.0009618505,0.001060735,0.001671486,0.003287558,0.006708828,0.0046763,0.003238526,0.003008306],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.001354086,"about_ca_system_score_gemma":0.001736764,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.001252214,"about_ca_topic_score_gemma":0.001930817,"domain_scores_codex":[0.9941889,0.001993487,0.0001933812,0.001693372,0.001505798,0.0004250215],"domain_scores_gemma":[0.9831883,0.007639284,0.001503662,0.002882759,0.00387498,0.0009109213],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"design_other","study_design_gemma":"not_applicable","study_design_scores_codex":[0.00174426,0.0008794131,0.06614889,0.008125256,0.0009068251,0.0003284331,0.001406033,0.004747438,0.1570022,0.08218811,0.02123043,0.6552927],"study_design_scores_gemma":[0.0003949374,0.002017932,0.04977114,0.003653582,0.0007027724,0.001913654,0.002209782,0.0123736,0.1105306,0.1839661,0.6317749,0.0006910876],"study_design_candidate":"not_applicable","study_design_consensus":null,"genre_codex":"review","genre_gemma":"review","genre_scores_codex":[0.09679222,0.6466204,0.168585,0.01458817,0.003645574,0.0003726142,0.005741285,0.002280968,0.06137389],"genre_scores_gemma":[0.5980018,0.1784033,0.191043,0.00633409,0.005166993,0.0009450317,0.005304495,0.000759773,0.01404151],"genre_candidate":"review","genre_consensus":"review","teacher_disagreement_score":0.01552114,"threshold_uncertainty_score":0.0820846,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02491396691603395,"score_gpt":0.2443034630185298,"score_spread":0.2193894961024959,"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."}}