{"id":"W2189021436","doi":"10.1140/epjb/e2018-90353-8","title":"Two-step melting of three-sublattice order in S = 1 easy-axis triangular lattice antiferromagnets","year":2018,"lang":"en","type":"article","venue":"The European Physical Journal B","topic":"Physics of Superconductivity and Magnetism","field":"Physics and Astronomy","cited_by":1,"is_retracted":false,"has_abstract":false,"ca_institutions":"University of Toronto","funders":"","keywords":"Antiferromagnetism; Anisotropy; Hexagonal lattice; Heisenberg model; Lattice (music); Monte Carlo method; Exponent; Series expansion; Phase transition; Order (exchange)","routes":{"ca_aff":true,"ca_fund":false,"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":[0.0009932513,0.0002250821,0.0003469668,0.0000649045,0.0002485185,0.00008678593,0.0006003809,0.00001523838,0.0001351443],"category_scores_gemma":[0.00004106077,0.0001639688,0.0001883213,0.0004042709,0.0003397416,0.0008692569,0.0002104343,0.0006331482,0.0002244458],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00001333498,"about_ca_system_score_gemma":0.0000514202,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0002002646,"about_ca_topic_score_gemma":0.00001351215,"domain_scores_codex":[0.9980535,0.0006069202,0.0003798895,0.0002406608,0.0003213223,0.0003977157],"domain_scores_gemma":[0.9988252,0.0002307591,0.0002292286,0.0003905655,0.000203637,0.0001206277],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"design_other","study_design_gemma":"theoretical_or_conceptual","study_design_scores_codex":[0.0003271015,0.002900163,0.004035088,0.00005193508,0.0005598342,0.0001128305,0.007379841,0.0003623036,0.2931235,0.1310894,0.001488651,0.5585694],"study_design_scores_gemma":[0.01856167,0.002895272,0.0730715,0.001048467,0.001016459,0.0001551382,0.005297166,0.01377596,0.04096645,0.8279198,0.012387,0.002905103],"study_design_candidate":"theoretical_or_conceptual","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.8495657,0.00005706312,0.001954807,0.0003108161,0.0002086204,0.0001304273,0.000009288187,0.00001635194,0.1477469],"genre_scores_gemma":[0.994603,0.000002209156,0.000728343,0.00006535673,0.004367478,0.000001512246,0.000002759479,0.00004345314,0.0001858735],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.6968305,"threshold_uncertainty_score":0.6686454,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02357901349271519,"score_gpt":0.2664680458742943,"score_spread":0.2428890323815792,"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."}}