{"id":"W4283708763","doi":"10.1016/j.nuclphysb.2022.115975","title":"Entanglement of inhomogeneous free fermions on hyperplane lattices","year":2022,"lang":"en","type":"article","venue":"Nuclear Physics B","topic":"Quantum many-body systems","field":"Physics and Astronomy","cited_by":18,"is_retracted":false,"has_abstract":true,"ca_institutions":"Université de Montréal","funders":"Natural Sciences and Engineering Research Council of Canada; Centre National de la Recherche Scientifique; Agence Nationale de la Recherche; Centre de Recherches Mathématiques; American Heart Association","keywords":"Quantum entanglement; Hyperplane; Eigenfunction; Conjecture; Fermion; Entropy (arrow of time); Physics; Operator (biology); Logarithm; Mathematical physics; Lattice (music); Quantum mechanics; Eigenvalues and eigenvectors; Mathematics; Statistical physics; Quantum; Pure mathematics; Combinatorics; Mathematical analysis","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":["insufficient_payload"],"consensus_categories":[],"category_scores_codex":[0.00009522247,0.0001320426,0.0002017253,0.00003471523,0.0002210495,0.00001968229,0.0003763427,0.00001194914,0.00178892],"category_scores_gemma":[0.000001754429,0.0001393455,0.0001124723,0.0001447672,0.00003445889,0.00004583385,0.0002655639,0.0001721742,0.0001546528],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00004083551,"about_ca_system_score_gemma":0.00002486115,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0002267497,"about_ca_topic_score_gemma":0.000001469955,"domain_scores_codex":[0.9989499,0.00007546576,0.0002094944,0.0002109654,0.0003541272,0.0002000653],"domain_scores_gemma":[0.9992101,0.00004443225,0.0001617085,0.0005080008,0.00002519693,0.00005060025],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"not_applicable","study_design_scores_codex":[0.00005982675,0.001260471,0.006897513,0.00003553618,0.0002428449,0.000009949984,0.001745143,0.002715459,0.01073515,0.9504639,0.01659428,0.009239923],"study_design_scores_gemma":[0.008704801,0.004568169,0.009209493,0.0002082653,0.0005502324,0.00002536944,0.01988274,0.04139392,0.02581314,0.1506977,0.7359158,0.003030278],"study_design_candidate":"theoretical_or_conceptual","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9651714,0.0000132862,0.00002882405,0.0001518772,0.0002986082,0.0002057236,0.0003956996,0.00004050729,0.03369408],"genre_scores_gemma":[0.9990506,3.7787e-7,0.00006412379,0.00008533314,0.0003497675,0.00002434616,0.00005612492,0.00004073427,0.0003285805],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.7997662,"threshold_uncertainty_score":0.9991236,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.0138552987791276,"score_gpt":0.2263083092509414,"score_spread":0.2124530104718138,"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."}}