{"id":"W4403335264","doi":"10.1103/physrevx.14.041011","title":"Planar Thermal Hall Effect from Phonons in Cuprates","year":2024,"lang":"en","type":"article","venue":"Physical Review X","topic":"Advanced Condensed Matter Physics","field":"Physics and Astronomy","cited_by":8,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of British Columbia; Canadian Institute for Advanced Research; Regroupement Québécois sur les Matériaux de Pointe; Université de Sherbrooke","funders":"Basic Energy Sciences; Fonds de recherche du Québec – Nature et technologies; Natural Sciences and Engineering Research Council of Canada; Office of Science; Canada First Research Excellence Fund; Agence Nationale de la Recherche; Canadian Institute for Advanced Research; Division of Materials Sciences and Engineering; Canada Foundation for Innovation; U.S. Department of Energy","keywords":"Cuprate; Condensed matter physics; Physics; Thermal Hall effect; Electron; Phonon; Planar; Hall effect; Magnetic field; Superconductivity; Quantum mechanics","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":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0001572006,0.0003535667,0.0002489428,0.0003852698,0.000378464,0.0006368576,0.0002777461,0.0002355732,0.00156488],"category_scores_gemma":[0.0004366758,0.0001934853,0.000145877,0.0002204169,0.0008313048,0.0004318023,0.0005425225,0.0003307891,0.0001618054],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0001992487,"about_ca_system_score_gemma":0.0001867411,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.000790989,"about_ca_topic_score_gemma":0.0008278847,"domain_scores_codex":[0.9998621,0.00001670417,0.000004602203,0.00002257281,0.00004766134,0.00004624714],"domain_scores_gemma":[0.9998121,0.00004375396,0.00004579048,0.00002604126,0.00003745931,0.00003494713],"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":[0.0005243356,0.00004879788,0.002227894,0.0004054229,0.0000378544,0.0005199015,0.0004297921,0.002202303,0.9774495,0.009360905,0.001063985,0.005729266],"study_design_scores_gemma":[0.0001125993,0.0005547462,0.01733229,0.00006707972,0.0000672156,0.0008067861,0.0006764714,0.01634017,0.9552227,0.004036282,0.004677692,0.0001059524],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9913489,0.0003946784,0.001853234,0.0001032282,0.00004005113,0.00001361366,0.000127011,0.0001814796,0.005937843],"genre_scores_gemma":[0.9989049,0.0001106843,0.0004719354,0.00002145157,0.00001025215,0.000006884763,0.00006836839,0.00001215805,0.0003932851],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.00156488,"threshold_uncertainty_score":0.005235076,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.007191229781596194,"score_gpt":0.3045307964492789,"score_spread":0.2973395666676827,"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."}}