{"id":"W2970743825","doi":"10.1175/jas-d-18-0274.1","title":"Climatological Features of the Weakly and Very Stably Stratified Nocturnal Boundary Layers. Part III: The Structure of Meteorological State Variables in Persistent Regime Nights and across Regime Transitions","year":2019,"lang":"en","type":"article","venue":"Journal of the Atmospheric Sciences","topic":"Wind and Air Flow Studies","field":"Environmental Science","cited_by":9,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of Victoria","funders":"Los Alamos National Laboratory; Natural Sciences and Engineering Research Council of Canada; National Oceanic and Atmospheric Administration; Universität Hamburg; Projektträger Jülich; Institut Polaire Français Paul Emile Victor; Canadian Network for Research and Innovation in Machining Technology, Natural Sciences and Engineering Research Council of Canada; Karlsruhe Institute of Technology","keywords":"Advection; Sunset; Atmospheric sciences; Boundary layer; Turbulence; Planetary boundary layer; Nocturnal; Kinetic energy; Sunrise; Environmental science; Geology; Climatology; Physics; Meteorology; Mechanics; Thermodynamics","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":[0.0001726415,0.00009713031,0.0001171776,0.0004042302,0.0001881161,0.0003596624,0.0001360183,0.0001517987,0.0007138719],"category_scores_gemma":[0.0004733149,0.0001043756,0.0001895814,0.0002388441,0.0001493095,0.0001416799,0.0002529072,0.000185802,0.00009524265],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0002063471,"about_ca_system_score_gemma":0.0001098461,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.009197543,"about_ca_topic_score_gemma":0.01259915,"domain_scores_codex":[0.9999614,0.000005817497,0.00000257685,0.00001102116,0.000006778654,0.00001242256],"domain_scores_gemma":[0.999728,0.00007015702,0.00007316077,0.00001757354,0.00004173101,0.00006933325],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"observational","study_design_gemma":"observational","study_design_scores_codex":[0.0003531159,0.0000662744,0.9539366,0.0000357807,0.00008534028,0.0001350476,0.000446897,0.003241799,0.0319896,0.0004698942,0.000444187,0.008795529],"study_design_scores_gemma":[0.000002044601,0.00001781634,0.9966409,0.000001671482,0.000003260913,0.00001201757,0.00006265876,0.002886465,0.000255781,0.00004471294,0.0000702734,0.000002451173],"study_design_candidate":"observational","study_design_consensus":"observational","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.999065,0.00002844677,0.0002307418,0.000009213912,0.000001682378,0.00000365181,0.0002854938,0.000008731145,0.0003670167],"genre_scores_gemma":[0.9994672,0.00000762531,0.0000886912,0.000002077947,0.000001180515,0.000002318352,0.0003539582,0.000001753251,0.00007519885],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.009197543,"threshold_uncertainty_score":0.01828802,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.009928751921470044,"score_gpt":0.2219268844933558,"score_spread":0.2119981325718858,"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."}}