{"id":"W2054488856","doi":"10.1063/1.4798391","title":"A statistical model approximation for perovskite solid-solutions: A Raman study of lead-zirconate-titanate single crystal","year":2013,"lang":"en","type":"article","venue":"Journal of Applied Physics","topic":"Ferroelectric and Piezoelectric Materials","field":"Materials Science","cited_by":40,"is_retracted":false,"has_abstract":true,"ca_institutions":"Simon Fraser University","funders":"","keywords":"Phase transition; Perovskite (structure); Phase boundary; Crystal (programming language); Ferroelectricity; Raman scattering; Phase (matter); Single crystal","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":[0.0003894756,0.0003511193,0.0004325541,0.0005278335,0.0004131755,0.0005873683,0.0007761214,0.0007028603,0.0008796406],"category_scores_gemma":[0.0007575459,0.0003047457,0.0005142245,0.0003118431,0.0006033363,0.0004812179,0.0003717515,0.0004698585,0.0002226619],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0004052422,"about_ca_system_score_gemma":0.0005519394,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.003006467,"about_ca_topic_score_gemma":0.002030003,"domain_scores_codex":[0.9998544,0.00003754907,0.000004549913,0.00002243,0.00005901256,0.0000219861],"domain_scores_gemma":[0.999762,0.0001185719,0.00003063619,0.0000209062,0.0000486774,0.00001928381],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"simulation_or_modeling","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.000128005,0.0002694523,0.003561379,0.0002795853,0.0001041864,0.000892458,0.0003404924,0.7257984,0.1365979,0.1230501,0.001572406,0.007405606],"study_design_scores_gemma":[0.000006180593,0.00001440956,0.0003896851,0.000002536619,0.000002546989,0.00002930472,0.00001910789,0.9941478,0.001455743,0.0037363,0.000191241,0.00000518562],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.8713024,0.001548544,0.1145099,0.000824917,0.00007772281,0.00007603504,0.0002548584,0.0002356257,0.01117002],"genre_scores_gemma":[0.9855165,0.0004684431,0.01057508,0.00007957561,0.00003100715,0.0000602241,0.0001693753,0.00005271266,0.003046997],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.003006467,"threshold_uncertainty_score":0.005977929,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.03420625025407957,"score_gpt":0.269835264040316,"score_spread":0.2356290137862365,"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."}}