{"id":"W1587374252","doi":"10.1063/1.4919614","title":"Relativistic Eulerian Vlasov simulations of the amplification of seed pulses by Brillouin backscattering in plasmas","year":2015,"lang":"en","type":"article","venue":"Physics of Plasmas","topic":"Laser-Plasma Interactions and Diagnostics","field":"Physics and Astronomy","cited_by":15,"is_retracted":false,"has_abstract":true,"ca_institutions":"Institut National de la Recherche Scientifique; Hydro-Québec","funders":"Natural Sciences and Engineering Research Council of Canada","keywords":"Physics; Pulse (music); Brillouin scattering; Plasma; Amplitude; Computational physics; Vlasov equation; Distribution function; Scattering; Raman amplification; Atomic physics; Optics; Raman scattering; Laser; Quantum mechanics; Raman spectroscopy","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":[0.0004871682,0.0005322554,0.0006598819,0.0005835309,0.0006646734,0.0007041965,0.001176445,0.001251139,0.002546542],"category_scores_gemma":[0.002488687,0.0004623587,0.0005392922,0.0006633252,0.0009226759,0.0005070855,0.0007886678,0.000862022,0.0001962552],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00150672,"about_ca_system_score_gemma":0.001377506,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.02248155,"about_ca_topic_score_gemma":0.008324068,"domain_scores_codex":[0.999804,0.00005190654,0.000007497098,0.00001412479,0.00004806356,0.00007452478],"domain_scores_gemma":[0.9987661,0.0007348957,0.0001423138,0.00005127965,0.0001550571,0.0001505147],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"simulation_or_modeling","study_design_gemma":"simulation_or_modeling","study_design_scores_codex":[0.00007016095,0.00003262918,0.001249612,0.00002446578,0.00001640244,0.00006651136,0.000076098,0.9925639,0.001400275,0.003634245,0.0001707383,0.0006949598],"study_design_scores_gemma":[0.00001860956,0.00001413459,0.0002322614,0.000003357868,0.000002774915,0.000005222264,0.0000142205,0.9987438,0.0003282205,0.000488298,0.0001446622,0.000004384542],"study_design_candidate":"simulation_or_modeling","study_design_consensus":"simulation_or_modeling","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9565078,0.0002301981,0.02777879,0.0004327121,0.00005873672,0.00005829297,0.00046404,0.0003055266,0.01416386],"genre_scores_gemma":[0.9888743,0.0001007082,0.00831426,0.00006641659,0.00001543633,0.0000921674,0.0002718223,0.000109052,0.002155707],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.02248155,"threshold_uncertainty_score":0.0447014,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02388850457589075,"score_gpt":0.2615396049864729,"score_spread":0.2376511004105822,"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."}}