{"id":"W3123538188","doi":"10.1103/physrevlett.127.277206","title":"Understanding Reentrance in Frustrated Magnets: The Case of the <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi>Er</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi>Sn</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">O</mml:mi></mml:mrow><mml:mrow><mml:mn>7</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math> Pyrochlore","year":2021,"lang":"lv","type":"article","venue":"Physical Review Letters","topic":"Advanced Condensed Matter Physics","field":"Physics and Astronomy","cited_by":16,"is_retracted":false,"has_abstract":true,"ca_institutions":"Canadian Institute for Advanced Research; University of Waterloo","funders":"Natural Sciences and Engineering Research Council of Canada; National Institute of Standards and Technology; University of Waterloo; Agence Nationale de la Recherche; Canada Research Chairs; Centre National de la Recherche Scientifique; Canadian Institute for Advanced Research; U.S. Department of Commerce; U.S. Department of Energy","keywords":"Phase diagram; Pyrochlore; Antiferromagnetism; Phase (matter); Reentrancy; Symmetry (geometry); Monte Carlo method; Thermal fluctuations","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":["metaepi_narrow","sts","scholarly_communication","open_science","research_integrity","insufficient_payload"],"consensus_categories":["metaepi_narrow","sts","research_integrity","insufficient_payload"],"category_scores_codex":[0.005669148,0.0034361,0.001356395,0.001761459,0.005037945,0.005022564,0.008805979,0.00528859,0.9522398],"category_scores_gemma":[0.004372736,0.00719342,0.008007996,0.006265959,0.007251123,0.005634035,0.007390282,0.007520886,0.00494083],"about_ca_system_candidate":true,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00008679278,"about_ca_system_score_gemma":0.006367444,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.005681951,"about_ca_topic_score_gemma":0.006523883,"domain_scores_codex":[0.9673518,0.002778101,0.006655632,0.006320354,0.007948761,0.00894535],"domain_scores_gemma":[0.9718779,0.006348293,0.008117172,0.008807932,0.0007316781,0.004117058],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"not_applicable","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.003817607,0.001270471,0.00004830551,0.00595589,0.00613949,0.007996809,0.003954964,0.0050293,0.009038545,0.1612252,0.7905172,0.005006253],"study_design_scores_gemma":[0.005908748,0.003225741,0.0002043967,0.007534517,0.007058622,0.004611982,0.005948252,0.008363581,0.9388626,0.0003715017,0.01138979,0.006520255],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"other","genre_gemma":"empirical","genre_scores_codex":[0.1400467,0.006642377,0.003687404,0.004997879,0.007118149,0.000181281,0.002084324,0.0006475427,0.8345944],"genre_scores_gemma":[0.9561468,0.007029728,0.003350186,0.009556429,0.007491037,0.005529932,0.00631586,0.003672883,0.0009071205],"genre_candidate":"empirical","genre_consensus":null,"teacher_disagreement_score":0.9472989,"threshold_uncertainty_score":0.9992656,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02346244697774271,"score_gpt":0.2524902275993817,"score_spread":0.229027780621639,"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."}}