{"id":"W1820722395","doi":"10.1038/nphys1109","title":"Linear temperature dependence of resistivity and change in the Fermi surface at the pseudogap critical point of a high-Tc superconductor","year":2008,"lang":"en","type":"article","venue":"Nature Physics","topic":"Physics of Superconductivity and Magnetism","field":"Physics and Astronomy","cited_by":240,"is_retracted":false,"has_abstract":false,"ca_institutions":"Canadian Institute for Advanced Research; Université de Sherbrooke","funders":"National High Magnetic Field Laboratory; Natural Sciences and Engineering Research Council of Canada; Canadian Institute for Advanced Research; Fonds Québécois de la Recherche sur la Nature et les Technologies; National Science Foundation","keywords":"Pseudogap; Condensed matter physics; Physics; Fermi surface; Superconductivity; Quantum critical point; Fermi liquid theory; Electrical resistivity and conductivity; Quantum oscillations; Fermi energy; High-temperature superconductivity; Cuprate; Quantum phase transition; Phase transition; Electron; 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":"codex-gemma-dda1882f352a","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0002424373,0.0002123564,0.0003461431,0.00001859626,0.0001930254,0.00001348287,0.0003222001,0.0001500149,0.00003508248],"category_scores_gemma":[0.00003608139,0.0001352426,0.0001121511,0.0002805667,0.0005467528,0.0007565265,0.0001659999,0.0009699569,0.000003034731],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00001491854,"about_ca_system_score_gemma":0.00006224211,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.001359117,"about_ca_topic_score_gemma":0.00009953722,"domain_scores_codex":[0.9987206,0.0001742355,0.0001996798,0.0003039075,0.0003507435,0.0002508734],"domain_scores_gemma":[0.9987646,0.0005222062,0.00006565312,0.0004607414,0.0001406643,0.0000461179],"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":[0.000186705,0.001659941,0.02009674,0.0002569167,0.0001287644,0.00002767068,0.01497821,0.00005972915,0.5123342,0.4463206,0.001475245,0.002475326],"study_design_scores_gemma":[0.002361903,0.0004264301,0.1802852,0.0002926335,0.0002164068,0.00004964884,0.002542004,0.0002175262,0.6336253,0.1784875,0.0004850582,0.001010347],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9960999,0.0007062145,0.00002431574,0.002266448,0.0001219333,0.000295597,0.0002447122,0.000007651536,0.0002332512],"genre_scores_gemma":[0.9990346,0.00004379218,0.0002224916,0.0001924536,0.0004046767,0.00001815616,0.00002562478,0.00001586002,0.00004236768],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.267833,"threshold_uncertainty_score":0.5515034,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02718336346953027,"score_gpt":0.2806644655530885,"score_spread":0.2534811020835582,"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."}}