{"id":"W2099965906","doi":"10.1103/physrevlett.114.045701","title":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>S</mml:mi><mml:mi>U</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>3</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow></mml:math>Semiclassical Representation of Quantum Dynamics of Interacting Spins","year":2015,"lang":"lv","type":"article","venue":"Physical Review Letters","topic":"Quantum many-body systems","field":"Physics and Astronomy","cited_by":58,"is_retracted":false,"has_abstract":true,"ca_institutions":"","funders":"Air Force Office of Scientific Research; Natural Sciences and Engineering Research Council of Canada; National Science Foundation","keywords":"Physics; Semiclassical physics; Hamiltonian (control theory); Formalism (music); Mott insulator; Parameter space; Superfluidity; Quantum mechanics; Quantum; Mathematical physics; Statistics; 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":["metaepi_narrow","insufficient_payload"],"consensus_categories":["insufficient_payload"],"category_scores_codex":[0.002009881,0.001195241,0.000952901,0.0003833028,0.0008131746,0.0009294755,0.002292066,0.000941599,0.003829967],"category_scores_gemma":[0.001683972,0.001941096,0.002917317,0.001393443,0.001603061,0.001670871,0.001853485,0.002245249,0.001637512],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00005232151,"about_ca_system_score_gemma":0.001073469,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.002333326,"about_ca_topic_score_gemma":0.000309012,"domain_scores_codex":[0.9887546,0.0008544541,0.003083865,0.002154574,0.002884129,0.002268401],"domain_scores_gemma":[0.9897186,0.002141874,0.004212605,0.002402819,0.0003399979,0.001184169],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"simulation_or_modeling","study_design_scores_codex":[0.0006935202,0.0007794494,0.00007382844,0.004122337,0.002021605,0.0003277491,0.00191732,0.001599996,0.006083978,0.9232101,0.05529235,0.003877807],"study_design_scores_gemma":[0.00264472,0.002315208,0.0001030112,0.0115885,0.004035722,0.0004342945,0.004324713,0.5163356,0.4466953,0.004249714,0.004542489,0.00273077],"study_design_candidate":"theoretical_or_conceptual","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9804968,0.00196892,0.002152464,0.002206924,0.00239392,0.0001544655,0.0007724515,0.0001795256,0.00967455],"genre_scores_gemma":[0.9897391,0.001167699,0.0008280877,0.001467146,0.003280329,0.0007638504,0.002034246,0.0006825469,0.0000370037],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.9189603,"threshold_uncertainty_score":0.9991398,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02403099704179036,"score_gpt":0.2786472747516971,"score_spread":0.2546162777099067,"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."}}