{"id":"W2530114778","doi":"10.1063/1.4964724","title":"Nonlinear excitation of long-wavelength modes in Hall plasmas","year":2016,"lang":"en","type":"article","venue":"Physics of Plasmas","topic":"Plasma Diagnostics and Applications","field":"Engineering","cited_by":10,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of Saskatchewan","funders":"Air Force Office of Scientific Research; Natural Sciences and Engineering Research Council of Canada; Russian Foundation for Basic Research","keywords":"Physics; Lower hybrid oscillation; Plasma; Instability; Magnetic field; Hall effect; Two-stream instability; Modulational instability; Upper hybrid oscillation; Excitation; Waves in plasmas; Condensed matter physics; Electron; Wavelength; Dispersion relation; Electromagnetic electron wave; Computational physics; Optics; Quantum mechanics","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":"codex-gemma-dda1882f352a","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.00005637558,0.0001109088,0.0001866629,0.00006251725,0.0000111315,0.000004331012,0.000127506,0.00005046202,0.000004849607],"category_scores_gemma":[0.0000483045,0.0000968603,0.00004676018,0.0001657802,0.00004794352,0.0001215123,0.00002068821,0.0000619365,0.00003075837],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0000286601,"about_ca_system_score_gemma":0.00001891795,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.00001703334,"about_ca_topic_score_gemma":0.00007412322,"domain_scores_codex":[0.9993306,0.000007529646,0.0002640164,0.0001168507,0.0001310161,0.0001499648],"domain_scores_gemma":[0.9992779,0.0003724867,0.00006509121,0.0001854417,0.00006100641,0.00003804474],"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":[0.00005878339,0.001079297,0.01351511,0.0006258948,0.0001996918,0.00001012293,0.001121291,0.2340073,0.4976826,0.1727975,0.000878229,0.07802424],"study_design_scores_gemma":[0.0007370032,0.00003802789,0.004430217,0.0001715897,0.00001773731,8.391685e-7,0.00003754591,0.2285095,0.7487159,0.01697027,0.0001651504,0.0002062061],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9879364,0.0000137729,0.009388709,0.00007626679,0.00004887213,0.0001130376,0.000159116,0.00003981005,0.002223974],"genre_scores_gemma":[0.9945546,0.0001302141,0.005177133,0.000002889343,0.00004404869,0.00002287788,0.00001923539,0.00002319595,0.00002582527],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.2510333,"threshold_uncertainty_score":0.3949848,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01506198886234988,"score_gpt":0.2196575800005346,"score_spread":0.2045955911381847,"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."}}