{"id":"W2029297993","doi":"10.1103/physreva.87.022711","title":"Polarization correlations for electron-impact excitation of the resonant transitions of Ne and Ar at low incident energies","year":2013,"lang":"en","type":"article","venue":"Physical Review A","topic":"Atomic and Molecular Physics","field":"Physics and Astronomy","cited_by":2,"is_retracted":false,"has_abstract":true,"ca_institutions":"York University; University of Windsor","funders":"Natural Sciences and Engineering Research Council of Canada; National Science Foundation","keywords":"Physics; Atomic physics; Neon; Excitation; Circular polarization; Scattering; Polarization (electrochemistry); Electron ionization; Electron; Linear polarization; Electron scattering; Excited state; Argon; Ionization; Quantum mechanics; Magnetic field","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":[0.00003608779,0.00007689882,0.0001877661,0.000009729433,0.00006257847,0.000004643618,0.00005270883,0.000009204939,0.00001215571],"category_scores_gemma":[0.000009368698,0.00005141769,0.0001749108,0.0001160437,0.00005029578,0.00008253896,0.00001964446,0.00004190078,0.000002025231],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00001559883,"about_ca_system_score_gemma":0.00004258045,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.00007722966,"about_ca_topic_score_gemma":0.000001090289,"domain_scores_codex":[0.9995381,0.00003307428,0.0001664593,0.00008741959,0.00008732471,0.00008768478],"domain_scores_gemma":[0.9995407,0.0000572666,0.0001484638,0.0001277407,0.00009897289,0.0000268829],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"bench_or_experimental","study_design_gemma":"theoretical_or_conceptual","study_design_scores_codex":[0.00002003837,0.0005582681,0.007078703,0.0009035493,0.0002195989,2.919751e-8,0.001485234,0.0006731204,0.4918636,0.4708135,0.001247979,0.02513644],"study_design_scores_gemma":[0.00255393,0.0006184126,0.3007654,0.004411081,0.001828106,0.000002024727,0.0003583543,0.06807125,0.2071568,0.4110003,0.002269613,0.000964694],"study_design_candidate":"theoretical_or_conceptual","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9686894,0.0009848805,0.02934564,0.0001918705,0.00001250263,0.0006144537,0.00003876416,0.000003629371,0.0001188782],"genre_scores_gemma":[0.999541,0.00009462894,0.00009324387,0.00004286659,0.00004154295,0.00008128099,0.00005830585,0.000008188867,0.0000388714],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.2936867,"threshold_uncertainty_score":0.2096753,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.006443619023290866,"score_gpt":0.2727785569252813,"score_spread":0.2663349379019904,"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."}}