{"id":"W2046868516","doi":"10.1103/physrevlett.93.213003","title":"Absolute Ionization Rates of Multielectron Transition Metal Atoms in Strong Infrared Laser Fields","year":2004,"lang":"en","type":"article","venue":"Physical Review Letters","topic":"Laser-Matter Interactions and Applications","field":"Physics and Astronomy","cited_by":56,"is_retracted":false,"has_abstract":true,"ca_institutions":"National Research Council Canada; Steacie Institute for Molecular Sciences","funders":"","keywords":"Atomic physics; Ionization; Infrared; Laser; Materials science; Far-infrared laser; Transition metal; Physics; Ion; Optics; Chemistry","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":[0.00004230837,0.0001074998,0.0002164886,0.00003349657,0.00003360532,0.00001215327,0.0000808309,0.000007129543,0.0001099841],"category_scores_gemma":[0.000002256351,0.00009629739,0.0001309977,0.000225766,0.00002514931,0.0001967141,0.00001058287,0.0001342377,0.00003877888],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00002792383,"about_ca_system_score_gemma":0.00001608412,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0001666398,"about_ca_topic_score_gemma":0.000006842698,"domain_scores_codex":[0.9993439,0.00002930021,0.0002409443,0.0001539137,0.00009222058,0.0001396906],"domain_scores_gemma":[0.9996628,0.00003217402,0.00009463555,0.0001507113,0.00002943603,0.00003023929],"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":[0.0001924246,0.01659006,0.009635408,0.005154945,0.001553882,0.00001519709,0.007369875,0.2550622,0.4509542,0.1398099,0.01834741,0.0953145],"study_design_scores_gemma":[0.0125372,0.0008482108,0.05866861,0.01440297,0.001786696,0.00000850422,0.0007550494,0.03924992,0.7731193,0.06246169,0.03209318,0.004068678],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9589082,0.0001069183,0.03630859,0.003794879,0.00002988529,0.0004378833,0.00002418093,0.00001398032,0.0003754772],"genre_scores_gemma":[0.998096,0.00005065397,0.0001621062,0.001302221,0.0000946279,0.0001518216,0.0001202017,0.000009840967,0.00001250598],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.3221651,"threshold_uncertainty_score":0.3926894,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01187487049361963,"score_gpt":0.2947511358715014,"score_spread":0.2828762653778818,"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."}}