{"id":"W2951996249","doi":"10.1103/physrevaccelbeams.21.103401","title":"Collisionless shock acceleration of narrow energy spread ion beams from mixed species plasmas using <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mn>1</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mi>μ</mml:mi><mml:mi mathvariant=\"normal\">m</mml:mi></mml:mrow></mml:math> lasers","year":2018,"lang":"lv","type":"article","venue":"Physical Review Accelerators and Beams","topic":"Laser-Plasma Interactions and Diagnostics","field":"Physics and Astronomy","cited_by":43,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of Alberta","funders":"Lawrence Livermore National Laboratory; Argonne National Laboratory; National Science Foundation; University of California, Los Angeles; Laboratory Directed Research and Development; Fusion Energy Sciences; U.S. Department of Energy; Natural Sciences and Engineering Research Council of Canada; National Nuclear Security Administration; Instituto Superior Técnico; Office of Science","keywords":"Ion; Plasma; Acceleration; Shock (circulatory); Laser; Shock wave; Spectral line; Beam (structure)","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":[0.0002425538,0.0002566565,0.0001783514,0.0003466113,0.0002844431,0.0003831102,0.0004958653,0.000311368,0.005416709],"category_scores_gemma":[0.0003305218,0.0002776016,0.0002245564,0.0004162194,0.0003040104,0.0003186041,0.0007094134,0.0004361733,0.0008245886],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.000541335,"about_ca_system_score_gemma":0.0003291003,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0007399219,"about_ca_topic_score_gemma":0.001439221,"domain_scores_codex":[0.9998903,0.00001268413,0.000005641166,0.00002517249,0.00004160625,0.00002460583],"domain_scores_gemma":[0.9998724,0.00003542379,0.00003147858,0.00001715563,0.00002505619,0.00001842595],"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":[0.0005953488,0.00004693384,0.00134626,0.0001193576,0.00005265963,0.000189137,0.0003682971,0.001032191,0.9807222,0.003572675,0.0009997833,0.01095522],"study_design_scores_gemma":[0.00007738866,0.0002533055,0.004404502,0.00001431761,0.000020768,0.0001737287,0.00008730957,0.004098458,0.9857759,0.0003856329,0.004692327,0.00001619517],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9652069,0.0006740417,0.01913279,0.0002635923,0.0000630932,0.00009902693,0.0003212962,0.0002581825,0.0139812],"genre_scores_gemma":[0.9782818,0.0004680541,0.009381559,0.00008036097,0.00001621496,0.00006873887,0.0003586372,0.00008724033,0.01125737],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.005416709,"threshold_uncertainty_score":0.01812077,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02172538229607673,"score_gpt":0.2597320962823108,"score_spread":0.238006713986234,"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."}}