{"id":"W3175733309","doi":"10.1103/physrevlett.128.036401","title":"Unconventional Hysteretic Transition in a Charge Density Wave","year":2022,"lang":"en","type":"article","venue":"Physical Review Letters","topic":"Organic and Molecular Conductors Research","field":"Materials Science","cited_by":36,"is_retracted":false,"has_abstract":true,"ca_institutions":"","funders":"SLAC National Accelerator Laboratory; U.S. Department of Energy; Division of Electrical, Communications and Cyber Systems; National Key Research and Development Program of China; Division of Materials Research; Office of Science; Army Research Office; Basic Energy Sciences; Canadian Light Source; Adolph C. and Mary Sprague Miller Institute for Basic Research in Science, University of California Berkeley; Gordon and Betty Moore Foundation; National Natural Science Foundation of China; Harvard University; Division of Materials Sciences and Engineering; National Science Foundation","keywords":"Charge density wave; Metastability; Hysteresis; Condensed matter physics; Phase transition; Charge ordering; Phase (matter); Modulation (music); Physics; Diffraction; Charge (physics); Symmetry (geometry); Materials science; Quantum mechanics; Superconductivity","routes":{"ca_aff":false,"ca_fund":true,"ca_venue":false,"about_ca":false,"invisible_to_affiliation_only":true},"retraction":null,"screen":null,"direct_labels":[],"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.00004006503,0.00008635179,0.00009357611,0.0001478066,0.0001833066,0.000275496,0.0002362065,0.0001788998,0.001189521],"category_scores_gemma":[0.0001793625,0.00009396006,0.00005393157,0.0001064073,0.0004699662,0.0003472379,0.0001989127,0.0002689968,0.0001235772],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00013373,"about_ca_system_score_gemma":0.00006887154,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.00009776079,"about_ca_topic_score_gemma":0.0001904925,"domain_scores_codex":[0.9999686,0.000002845563,0.000001648531,0.000007381399,0.00001349462,0.000006016461],"domain_scores_gemma":[0.9999182,0.00002645666,0.00001890307,0.00001990968,0.00000897689,0.000007476291],"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":[0.00007622548,0.00002548259,0.001451157,0.00008002375,0.000008925562,0.0005221346,0.0001288632,0.0006486281,0.9795755,0.01040162,0.0003242347,0.006757239],"study_design_scores_gemma":[0.00003308852,0.0003733284,0.02306741,0.00002589397,0.00001484157,0.002302907,0.0003466997,0.04348182,0.9067012,0.01596609,0.007640339,0.00004649907],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9906487,0.0002549227,0.005257959,0.0001233013,0.00002267607,0.000006690899,0.00008571435,0.0001768165,0.003423219],"genre_scores_gemma":[0.9985202,0.00004655362,0.0008515017,0.00001803675,0.000003788977,0.000005563048,0.00003281453,0.000007537451,0.0005139705],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.001189521,"threshold_uncertainty_score":0.003979385,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.0303007651123115,"score_gpt":0.2920944842888322,"score_spread":0.2617937191765207,"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."}}