{"id":"W2055601610","doi":"10.1016/j.physc.2004.03.132","title":"Raman spectra in chiral superconductors","year":2004,"lang":"en","type":"article","venue":"Physica C Superconductivity","topic":"Advanced Condensed Matter Physics","field":"Physics and Astronomy","cited_by":2,"is_retracted":false,"has_abstract":false,"ca_institutions":"University of Toronto","funders":"","keywords":"Raman spectroscopy; Superconductivity; Physics; Condensed matter physics; Symmetry (geometry); Spectral line; Signature (topology); Momentum (technical analysis); Resonance (particle physics); Quantum mechanics; Mathematics","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":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.00009611413,0.0003979911,0.0004670782,0.0001125609,0.0001211826,0.00005851025,0.0003291774,0.00004760753,0.0003271459],"category_scores_gemma":[0.000006884189,0.0004161244,0.0002084873,0.0004743011,0.0001922809,0.001684703,0.0001143628,0.0005472465,0.0002745974],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0001574841,"about_ca_system_score_gemma":0.0001308203,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.001068653,"about_ca_topic_score_gemma":0.00003625929,"domain_scores_codex":[0.9980579,0.00006579141,0.000287842,0.0006648307,0.0002517875,0.0006718214],"domain_scores_gemma":[0.9990627,0.00005702856,0.00005477451,0.0006368681,0.00004601273,0.0001426621],"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":[0.00002087182,0.001466665,0.0171313,0.00002545648,0.00008775137,0.00001639918,0.002461302,0.001278553,0.7149209,0.2591216,0.00008972519,0.003379509],"study_design_scores_gemma":[0.002182758,0.00006839451,0.01135591,0.00005087671,0.00003015263,0.00000347534,0.001367574,0.00002345119,0.3463407,0.6374176,0.0003049679,0.0008541998],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9890249,0.00001592441,0.001844522,0.0005358467,0.000270386,0.0003185822,0.00003553332,0.0001109485,0.007843319],"genre_scores_gemma":[0.9979466,9.726323e-7,0.001053438,0.00008274564,0.000621793,0.00006319087,0.00003569535,0.00006296831,0.0001325531],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.378296,"threshold_uncertainty_score":0.9998291,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01387498767926653,"score_gpt":0.2524388804809991,"score_spread":0.2385638928017326,"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."}}