{"id":"W2021626435","doi":"10.1103/physreva.77.032705","title":"Strong nonmonopole shake transitions in the Br<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mn>3</mml:mn><mml:msup><mml:mi>d</mml:mi><mml:mrow><mml:mo>−</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mi>n</mml:mi><mml:mi>p</mml:mi><mml:mi>π</mml:mi></mml:mrow></mml:mrow></mml:math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn>6</mml:mn><mml:mo>–</mml:mo><mml:mn>9</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math>resonant Auger spectra of HBr","year":2008,"lang":"lv","type":"article","venue":"Physical Review A","topic":"Atomic and Molecular Physics","field":"Physics and Astronomy","cited_by":10,"is_retracted":false,"has_abstract":true,"ca_institutions":"Western University; Canadian Light Source (Canada); University of Saskatchewan","funders":"","keywords":"Physics; Excited state; Rydberg formula; Atomic physics; Auger; Spectral line; Auger electron spectroscopy; Ionization; Quantum mechanics","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":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0007390614,0.0005988474,0.00111523,0.001207091,0.002687163,0.003314758,0.001382834,0.001790487,0.0696656],"category_scores_gemma":[0.002449593,0.0006382494,0.001029516,0.0009032169,0.001640063,0.0047579,0.002931474,0.002398905,0.00778554],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.001538433,"about_ca_system_score_gemma":0.001285024,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.002081382,"about_ca_topic_score_gemma":0.004515051,"domain_scores_codex":[0.9994038,0.0001048461,0.00002336847,0.0001350519,0.000141514,0.0001913626],"domain_scores_gemma":[0.9991861,0.0002703757,0.00006347033,0.0002101984,0.0001132831,0.0001565009],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.0002360166,0.0001091551,0.0003373899,0.0001774391,0.00002668221,0.0002493804,0.0002436777,0.005768802,0.006025737,0.9533624,0.02274237,0.010721],"study_design_scores_gemma":[0.0001364818,0.0001044307,0.0007623599,0.00008625124,0.00002147817,0.0001674338,0.0003084673,0.08765156,0.005755116,0.876401,0.0285261,0.00007930242],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"other","genre_gemma":"empirical","genre_scores_codex":[0.2653893,0.002135888,0.2035801,0.005934934,0.002365461,0.0002774053,0.001772638,0.003397186,0.515147],"genre_scores_gemma":[0.8755759,0.0005963519,0.02462529,0.001139194,0.0001711737,0.0002846339,0.0007007783,0.0011396,0.09576707],"genre_candidate":"empirical","genre_consensus":null,"teacher_disagreement_score":0.0696656,"threshold_uncertainty_score":0.2330547,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01847433944543259,"score_gpt":0.2513653187462452,"score_spread":0.2328909793008126,"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."}}