{"id":"W2768303468","doi":"10.1103/physrevlett.120.136801","title":"Competing Charge Density Waves Probed by Nonlinear Transport and Noise in the Second and Third Landau Levels","year":2018,"lang":"en","type":"article","venue":"Physical Review Letters","topic":"Quantum and electron transport phenomena","field":"Physics and Astronomy","cited_by":24,"is_retracted":false,"has_abstract":true,"ca_institutions":"McGill University; Université de Sherbrooke","funders":"Fonds de recherche du Québec – Nature et technologies; Natural Sciences and Engineering Research Council of Canada; Canada Foundation for Innovation; Canadian Institute for Advanced Research; Ministère du Développement Économique, de l’Innovation et de l’Exportation; Canada Excellence Research Chairs, Government of Canada; Gordon and Betty Moore Foundation; National Science Foundation","keywords":"Landau quantization; Condensed matter physics; Physics; Noise (video); Quantum Hall effect; Charge density wave; Magnetic field; Charge density; Electron; Charge (physics); Nonlinear system; 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":[0.0001597693,0.0001760307,0.0002081774,0.0004248431,0.0002312781,0.0005153298,0.0002462824,0.0002801226,0.0007954384],"category_scores_gemma":[0.0004476215,0.0001772438,0.0001023699,0.0002985294,0.000746747,0.0004829498,0.0003179274,0.0003472678,0.00009190954],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0004189037,"about_ca_system_score_gemma":0.0001596522,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0008964676,"about_ca_topic_score_gemma":0.0009388747,"domain_scores_codex":[0.9998928,0.00001323648,0.000003627439,0.0000201452,0.00003891906,0.00003124289],"domain_scores_gemma":[0.99966,0.0001697345,0.00007476845,0.00001895557,0.0000364962,0.00004008523],"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":[0.0002941875,0.00005013782,0.005685474,0.0000408676,0.00001011051,0.0001708419,0.0002056052,0.001148802,0.9848337,0.004360206,0.00004432376,0.003155706],"study_design_scores_gemma":[0.00004682328,0.0004682468,0.0355068,0.00001620418,0.0000283713,0.0004958404,0.000377188,0.07540323,0.8823416,0.004653259,0.0006182633,0.00004408782],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.997983,0.00006290543,0.001195277,0.00001903125,0.000001785428,0.000003077855,0.00001391869,0.00001288304,0.0007080775],"genre_scores_gemma":[0.9992602,0.00002849328,0.0004227558,0.00000555061,0.000001396622,0.000005182192,0.00001356787,0.00000360643,0.0002590791],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.0008964676,"threshold_uncertainty_score":0.00303936,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01138634848380612,"score_gpt":0.2490600616003932,"score_spread":0.237673713116587,"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."}}