{"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":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.002604055,0.0005463012,0.0005992742,0.0006953087,0.003892304,0.005350209,0.003057039,0.005067104,0.01300166],"category_scores_gemma":[0.00915074,0.0009340277,0.0007631617,0.000455266,0.009856048,0.01702168,0.003434068,0.003328554,0.001728378],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.003747871,"about_ca_system_score_gemma":0.001295752,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.00846584,"about_ca_topic_score_gemma":0.008382145,"domain_scores_codex":[0.9987477,0.0004330753,0.00002957883,0.0002943949,0.0002516823,0.000243595],"domain_scores_gemma":[0.9972875,0.001394325,0.0002517867,0.0005246426,0.0003272363,0.0002144734],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.000134691,0.00003466532,0.001025,0.0001804799,0.00001929546,0.003813237,0.0184805,0.003996445,0.003483926,0.9395116,0.01448432,0.01483588],"study_design_scores_gemma":[0.00004696754,0.00004937181,0.001072394,0.0001186509,0.00002429233,0.00268778,0.01006614,0.03727187,0.003352599,0.8530702,0.09215777,0.0000820247],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"other","genre_gemma":"empirical","genre_scores_codex":[0.2475593,0.004850601,0.2677531,0.05506568,0.0008929775,0.0001308027,0.0003419654,0.002208925,0.4211966],"genre_scores_gemma":[0.9200132,0.0009262588,0.04414097,0.001642993,0.0001347531,0.00006480809,0.0001412057,0.0006851464,0.03225067],"genre_candidate":"empirical","genre_consensus":null,"teacher_disagreement_score":0.01300166,"threshold_uncertainty_score":0.04349488,"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."}}