{"id":"W2032525003","doi":"10.1103/physrevb.89.104519","title":"Tuning between singlet, triplet, and mixed pairing states in an extended Hubbard chain","year":2014,"lang":"en","type":"article","venue":"Physical Review B","topic":"Physics of Superconductivity and Magnetism","field":"Physics and Astronomy","cited_by":28,"is_retracted":false,"has_abstract":true,"ca_institutions":"","funders":"Materials Research Science and Engineering Center, Harvard University; Ministero dello Sviluppo Economico; California NanoSystems Institute; Army Research Office; Institut Périmètre de physique théorique; Division of Materials Research; Hong Kong University of Science and Technology; National Science Foundation; Government of Canada; Industry Canada; Defense Advanced Research Projects Agency; University of Cincinnati","keywords":"Pairing; Physics; Singlet state; Hamiltonian (control theory); Fermion; Quantum mechanics; Hubbard model; Condensed matter physics; Topology (electrical circuits); Superconductivity; Excited state; Mathematics","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":"codex-gemma-dda1882f352a","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0003586294,0.0002154877,0.0005738867,0.00003538953,0.00008353346,0.00004769511,0.0001575418,0.0000177224,0.00002589781],"category_scores_gemma":[0.00002436141,0.0002016296,0.0001021794,0.0001641099,0.0000787457,0.0008942441,0.00009303982,0.0002512573,0.00001939863],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00001213255,"about_ca_system_score_gemma":0.00001599705,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0001299439,"about_ca_topic_score_gemma":0.000008462705,"domain_scores_codex":[0.9987118,0.0002121981,0.0002357927,0.0003656753,0.0001473689,0.0003271211],"domain_scores_gemma":[0.9992602,0.0002125048,0.0000728007,0.0002686491,0.00002836064,0.0001574294],"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":[0.000005492497,0.0004185076,0.00870884,0.0004774634,0.00003522758,0.000001207349,0.0004361473,0.00001706184,0.01420485,0.05441408,0.00007185825,0.9212093],"study_design_scores_gemma":[0.002481245,0.0006780517,0.05644486,0.00378178,0.0002991925,9.959685e-7,0.0003488728,0.006115326,0.006689996,0.8955879,0.02589484,0.001676957],"study_design_candidate":"theoretical_or_conceptual","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9946938,0.001111989,0.002062578,0.0005660965,0.00003601243,0.000257077,0.00001437903,0.00003584386,0.001222295],"genre_scores_gemma":[0.998751,0.0002160757,0.0001967156,0.0001664743,0.0005308306,0.00004050164,0.000058065,0.00002295358,0.00001738222],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.9195323,"threshold_uncertainty_score":0.8222216,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02676820812217631,"score_gpt":0.2942978247248768,"score_spread":0.2675296166027005,"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."}}