{"id":"W4254850864","doi":"10.1063/1.3257690","title":"Oscillator strengths and line widths of dipole-allowed transitions in N142 between 86.0 and 89.7 nm","year":2009,"lang":"en","type":"article","venue":"The Journal of Chemical Physics","topic":"Atmospheric Ozone and Climate","field":"Earth and Planetary Sciences","cited_by":19,"is_retracted":false,"has_abstract":true,"ca_institutions":"Steacie Institute for Molecular Sciences","funders":"","keywords":"Atomic physics; Dipole; Physics; Rydberg formula; Sigma; Radiative transfer; Line (geometry); Valence (chemistry); Optics; Ionization; Quantum mechanics","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":[],"consensus_categories":[],"category_scores_codex":[0.0001686655,0.00007513506,0.0002142222,0.000005525624,0.00002647875,0.000009061016,0.00009279753,0.00003610938,0.00003671294],"category_scores_gemma":[0.00002013541,0.00004740004,0.00003718917,0.0001150929,0.0001059306,0.0001168683,0.000004306798,0.0001804894,0.000001313685],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00000196445,"about_ca_system_score_gemma":0.0000190533,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.00003074398,"about_ca_topic_score_gemma":0.000006066433,"domain_scores_codex":[0.999401,0.00002882943,0.0002493297,0.00005267259,0.0001522762,0.0001158691],"domain_scores_gemma":[0.9995111,0.0001997453,0.0001244261,0.00006119413,0.00002612885,0.00007744927],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"design_other","study_design_gemma":"observational","study_design_scores_codex":[0.001074636,0.0004225202,0.2737354,0.0001456956,0.000269982,0.00003139805,0.00754413,0.002554306,0.1466552,0.0003674067,0.0008134422,0.5663858],"study_design_scores_gemma":[0.005182189,0.00228067,0.8200985,0.0004632143,0.0007141742,0.000127761,0.001813053,0.0092486,0.06620055,0.09214602,0.000939108,0.0007861229],"study_design_candidate":"observational","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.998015,0.0005334744,0.00008994612,0.000873738,0.00001523266,0.00003169988,0.00002134278,0.000002558796,0.0004169944],"genre_scores_gemma":[0.9991421,0.0002411872,0.0003631749,0.00009873171,0.0001435569,1.963631e-8,0.000003925381,0.000001557781,0.000005754559],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.5655997,"threshold_uncertainty_score":0.1932918,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.00881612861888368,"score_gpt":0.2290283511503398,"score_spread":0.2202122225314561,"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."}}