{"meta":{"page":1,"per_page":50,"max_per_page":100,"total":6,"total_is_capped":false,"direct_labels_cover":0,"predictions_cover":6,"direct_label_status":"direct model label, unvalidated","prediction_status":"machine_predicted_unvalidated (Codex and Gemma teacher distillation)","score_status":"score_only:v0-immature-baseline (scores rank; they never assert a category)","snapshot":{"source":"OpenAlex, pinned release, all 482 partitions","release":"2026-06-24","frame_built":"2026-07-12","author_layer_release":"2026-06-26"},"query_hash":"8c45e65bdc2a","filters":{"venue":"Proceedings of XXIIIrd International Symposium on Lattice Field Theory — PoS(LAT2005)"}},"results":[{"id":"W2944107673","doi":"10.22323/1.020.0245","title":"Three Dimensional N=2 Supersymmetry on the Lattice","year":2005,"lang":"en","type":"article","venue":"Proceedings of XXIIIrd International Symposium on Lattice Field Theory — PoS(LAT2005)","topic":"Quantum Chromodynamics and Particle Interactions","field":"Physics and Astronomy","cited_by":10,"is_retracted":false,"has_abstract":true,"routes":{"ca_aff":true,"ca_fund":false,"ca_venue":false,"about_ca":false},"ca_institutions":"McGill University","funders":"","keywords":"Supersymmetry; Physics; Lattice (music); Supersymmetry breaking; Lattice QCD; Particle physics; Lattice field theory; Theoretical physics; Lattice model (finance); Lattice constant; Limit (mathematics); Quantum chromodynamics; Quantum mechanics; Mathematics; Mathematical analysis","authors":[{"name":"Joshua B. Elliott","is_ca":true},{"name":"Guy D. Moore","is_ca":true}],"retraction":null,"screen_n_in":null,"score":{"opus":0.01021691403155264,"gpt":0.256458825490637,"spread":0.2462419114590844,"validation_status":"score_only:v0-immature-baseline"},"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0005568402,0.0006108452,0.0007522323,0.0005018151,0.001699996,0.002406923,0.0009048855,0.0005958751,0.004430883],"category_scores_gemma":[0.001111005,0.0004152202,0.0006676668,0.0007184113,0.002543324,0.001595194,0.001566906,0.00155566,0.0009990637],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0007568309,"about_ca_system_score_gemma":0.0007505771,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.002722926,"about_ca_topic_score_gemma":0.003307729,"domain_scores_codex":[0.9995529,0.0001426162,0.00002030046,0.00003206239,0.0001675439,0.0000846625],"domain_scores_gemma":[0.999539,0.0001311035,0.00006571134,0.0001065738,0.00005889776,0.00009880748],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"theoretical_or_conceptual","study_design_scores_codex":[0.0001609684,0.000123463,0.0005093099,0.00005474636,0.00001781949,0.0003901525,0.0002362474,0.03344952,0.004058964,0.9506805,0.003075483,0.007242803],"study_design_scores_gemma":[0.0001179556,0.00006419627,0.0002041531,0.00002245079,0.000008838261,0.0001125536,0.00009641331,0.182497,0.001835492,0.8103091,0.004693887,0.00003799558],"study_design_candidate":"theoretical_or_conceptual","study_design_consensus":"theoretical_or_conceptual","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.6855195,0.0008719961,0.1147442,0.002256538,0.000885164,0.00007142087,0.0002911853,0.000923342,0.1944367],"genre_scores_gemma":[0.9536591,0.0005516774,0.03457496,0.0003523678,0.0001724012,0.00008849037,0.0001839713,0.0001449711,0.01027198],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.004430883,"threshold_uncertainty_score":0.01482278,"prediction_status":"machine_predicted_unvalidated"},"labels":[],"label_agreement":null},{"id":"W1880996807","doi":"10.22323/1.020.0058","title":"Two Loop Partially Quenched and Finite Volume Chiral Perturbation Theory Results","year":2005,"lang":"en","type":"article","venue":"Proceedings of XXIIIrd International Symposium on Lattice Field Theory — PoS(LAT2005)","topic":"Quantum Chromodynamics and Particle Interactions","field":"Physics and Astronomy","cited_by":2,"is_retracted":false,"has_abstract":true,"routes":{"ca_aff":true,"ca_fund":false,"ca_venue":false,"about_ca":false},"ca_institutions":"Institute of Particle Physics","funders":"European Commission","keywords":"Chiral perturbation theory; Physics; Finite volume method; Quark; Meson; Lattice QCD; Quantum chromodynamics; Particle physics; Loop (graph theory); Lattice (music); Sigma; Quantum electrodynamics; Perturbation theory (quantum mechanics); Perturbation (astronomy); Quantum mechanics; Mathematics","authors":[{"name":"Johan Bijnens","is_ca":true},{"name":"Niclas Danielsson","is_ca":false},{"name":"Karim Ghorbani","is_ca":true},{"name":"Timo A. Lähde","is_ca":false}],"retraction":null,"screen_n_in":null,"score":{"opus":0.007706444818556794,"gpt":0.2599413405046155,"spread":0.2522348956860587,"validation_status":"score_only:v0-immature-baseline"},"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0005521691,0.0006013044,0.000716901,0.0008018914,0.0008677155,0.001204707,0.001365341,0.0009354522,0.004823121],"category_scores_gemma":[0.002184883,0.000249843,0.0008815432,0.000470544,0.002169435,0.001325412,0.001117312,0.001195096,0.0004514582],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0009767369,"about_ca_system_score_gemma":0.0008319225,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.002894864,"about_ca_topic_score_gemma":0.002052664,"domain_scores_codex":[0.9992998,0.0001708527,0.00001647157,0.0000700954,0.0002840234,0.0001588309],"domain_scores_gemma":[0.998957,0.0003787678,0.0001230915,0.0001905758,0.0001910282,0.0001594106],"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":[0.0002380762,0.0001677843,0.001440706,0.0001317355,0.00003926035,0.000716272,0.0003423588,0.1637467,0.0248523,0.8001006,0.001227873,0.006996293],"study_design_scores_gemma":[0.00008108171,0.00006571152,0.001200931,0.00002194441,0.00002388208,0.0002532043,0.00006760728,0.5768509,0.01101538,0.4094827,0.000890423,0.0000462065],"study_design_candidate":"simulation_or_modeling","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.8188439,0.0006134898,0.1103066,0.0009801561,0.0001291951,0.00005875729,0.0003639946,0.001971717,0.06673212],"genre_scores_gemma":[0.9904806,0.00009616256,0.005456773,0.0001158424,0.00003704195,0.00002946746,0.0001067412,0.0001427097,0.003534607],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.004823121,"threshold_uncertainty_score":0.01613492,"prediction_status":"machine_predicted_unvalidated"},"labels":[],"label_agreement":null},{"id":"W2963133425","doi":"10.22323/1.020.0038","title":"Automated Methods in Chiral Perturbation Theory on the Lattice","year":2005,"lang":"en","type":"article","venue":"Proceedings of XXIIIrd International Symposium on Lattice Field Theory — PoS(LAT2005)","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":1,"is_retracted":false,"has_abstract":true,"routes":{"ca_aff":true,"ca_fund":true,"ca_venue":false,"about_ca":false},"ca_institutions":"University of Regina","funders":"Natural Sciences and Engineering Research Council of Canada","keywords":"Feynman diagram; Lattice (music); Chiral perturbation theory; Perturbation (astronomy); Computer science; Algorithm; Statistical physics; Mathematics; Physics; Mathematical physics; Quantum mechanics; Quantum chromodynamics","authors":[{"name":"Georg von Hippel","is_ca":true},{"name":"B. Borasoy","is_ca":false},{"name":"H. Krebs","is_ca":false},{"name":"Randy Lewis","is_ca":true}],"retraction":null,"screen_n_in":null,"score":{"opus":0.01279231956502676,"gpt":0.3148140482171108,"spread":0.3020217286520841,"validation_status":"score_only:v0-immature-baseline"},"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.002842142,0.001274684,0.001343004,0.002130069,0.001719358,0.003059276,0.003225074,0.001252464,0.01140893],"category_scores_gemma":[0.009748658,0.0009960595,0.001548987,0.001814372,0.002623167,0.002900061,0.002893618,0.002767569,0.004128399],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.001465434,"about_ca_system_score_gemma":0.001921285,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.003139427,"about_ca_topic_score_gemma":0.003268462,"domain_scores_codex":[0.9961825,0.001666576,0.0002386167,0.0003078276,0.001414725,0.0001898148],"domain_scores_gemma":[0.9945075,0.003469057,0.000237156,0.001041012,0.0006446798,0.0001006305],"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":[0.0001216753,0.0001777565,0.0004707708,0.0004299548,0.00009048316,0.000364172,0.0003951252,0.1642912,0.005228361,0.5480237,0.007344313,0.2730624],"study_design_scores_gemma":[0.00007532952,0.00001659682,0.00005578918,0.00004701819,0.000008982734,0.00006055674,0.00004515026,0.4378603,0.003288462,0.5482588,0.0102537,0.00002928377],"study_design_candidate":"simulation_or_modeling","study_design_consensus":null,"genre_codex":"methods","genre_gemma":"methods","genre_scores_codex":[0.001468837,0.0001198483,0.9938686,0.0001142553,0.00003622834,0.00004124602,0.00006355427,0.00180178,0.002485598],"genre_scores_gemma":[0.04468064,0.0002024225,0.9519237,0.00007365541,0.00005677618,0.0002276256,0.0002142653,0.0008977879,0.0017231],"genre_candidate":"methods","genre_consensus":"methods","teacher_disagreement_score":0.01140893,"threshold_uncertainty_score":0.03816664,"prediction_status":"machine_predicted_unvalidated"},"labels":[],"label_agreement":null},{"id":"W2789367494","doi":"10.22323/1.020.0251","title":"Simulations of the F model on planar phi-4 Feynman diagrams","year":2005,"lang":"en","type":"article","venue":"Proceedings of XXIIIrd International Symposium on Lattice Field Theory — PoS(LAT2005)","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":0,"is_retracted":false,"has_abstract":false,"routes":{"ca_aff":true,"ca_fund":false,"ca_venue":false,"about_ca":false},"ca_institutions":"University of Waterloo","funders":"","keywords":"Feynman diagram; Planar; Computer science; Physics; Statistical physics; Mathematical physics; Computer graphics (images)","authors":[{"name":"Wolfhard Janke","is_ca":true},{"name":"Martin Weigel","is_ca":true}],"retraction":null,"screen_n_in":null,"score":{"opus":0.01046720735776349,"gpt":0.2632249756272574,"spread":0.252757768269494,"validation_status":"score_only:v0-immature-baseline"},"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0006739888,0.000800951,0.001732674,0.001396327,0.001900157,0.001852405,0.001983262,0.002626281,0.008954545],"category_scores_gemma":[0.003321626,0.0006611405,0.001031147,0.001426983,0.001650364,0.001549941,0.0009925989,0.001834452,0.00041408],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.002658267,"about_ca_system_score_gemma":0.001484876,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.02387801,"about_ca_topic_score_gemma":0.01241853,"domain_scores_codex":[0.9995509,0.0001361405,0.00001084457,0.00004116773,0.00006336394,0.0001975006],"domain_scores_gemma":[0.9981024,0.00100665,0.0001390631,0.0001390691,0.0002303827,0.000382523],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"simulation_or_modeling","study_design_gemma":"simulation_or_modeling","study_design_scores_codex":[0.0008329494,0.000356374,0.003082779,0.0001415362,0.0001141432,0.0006176751,0.0003841151,0.8916312,0.003389035,0.09172276,0.004874203,0.002853308],"study_design_scores_gemma":[0.0002042609,0.00007290666,0.0006084563,0.00001912867,0.00001645256,0.0000288812,0.0001099356,0.9857821,0.0007832533,0.0117909,0.0005588133,0.00002484966],"study_design_candidate":"simulation_or_modeling","study_design_consensus":"simulation_or_modeling","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9699646,0.0002244554,0.00346955,0.0007332916,0.0001371579,0.00004204172,0.0005578916,0.0003800423,0.024491],"genre_scores_gemma":[0.9959933,0.00006595529,0.001868658,0.00008317747,0.00002350856,0.0000372833,0.0003120514,0.00009686538,0.001519128],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.02387801,"threshold_uncertainty_score":0.04747802,"prediction_status":"machine_predicted_unvalidated"},"labels":[],"label_agreement":null},{"id":"W2791230469","doi":"10.22323/1.020.0254","title":"Classical simulation of quantum lambda phi^4","year":2005,"lang":"en","type":"article","venue":"Proceedings of XXIIIrd International Symposium on Lattice Field Theory — PoS(LAT2005)","topic":"Quantum Computing Algorithms and Architecture","field":"Computer Science","cited_by":0,"is_retracted":false,"has_abstract":true,"routes":{"ca_aff":true,"ca_fund":false,"ca_venue":false,"about_ca":false},"ca_institutions":"York University; University of Toronto","funders":"","keywords":"Lambda; Quantum; Computer science; Physics; Quantum mechanics","authors":[{"name":"Tzahi Yavin","is_ca":true},{"name":"Takayuki Hirayama","is_ca":true},{"name":"Bob Holdom","is_ca":true},{"name":"Roman Koniuk","is_ca":true}],"retraction":null,"screen_n_in":null,"score":{"opus":0.008967489440551098,"gpt":0.2591824212465664,"spread":0.2502149318060153,"validation_status":"score_only:v0-immature-baseline"},"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0005582402,0.0002131059,0.0003623784,0.0002735513,0.000568954,0.0006476676,0.001160902,0.0006266521,0.004083646],"category_scores_gemma":[0.0016495,0.0002475447,0.0002393459,0.0003380478,0.001060024,0.0007618879,0.0006539268,0.0007372997,0.0001354947],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.001152142,"about_ca_system_score_gemma":0.0008251911,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.007185926,"about_ca_topic_score_gemma":0.004755807,"domain_scores_codex":[0.9997938,0.00007186602,0.000005671097,0.00002723682,0.00004930653,0.00005199748],"domain_scores_gemma":[0.9991079,0.0005061375,0.00005245897,0.0000859409,0.0001300893,0.000117494],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"simulation_or_modeling","study_design_gemma":"simulation_or_modeling","study_design_scores_codex":[0.0003853412,0.0002634964,0.003381104,0.00006434732,0.00006710118,0.0002542288,0.0002406508,0.9262941,0.004352951,0.0584656,0.0009396023,0.005291416],"study_design_scores_gemma":[0.00001817181,0.00002708992,0.0001533411,0.000001506156,0.000002122049,0.000005946021,0.00001767141,0.9965205,0.0006906899,0.002396455,0.0001614327,0.00000516415],"study_design_candidate":"simulation_or_modeling","study_design_consensus":"simulation_or_modeling","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9675199,0.00005105243,0.02196855,0.0002981996,0.00004159636,0.00003560956,0.0001205605,0.0002460706,0.009718399],"genre_scores_gemma":[0.9891161,0.00002485156,0.00937726,0.00004593289,0.000006108799,0.00003548041,0.000085113,0.00002972659,0.001279303],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.007185926,"threshold_uncertainty_score":0.01428825,"prediction_status":"machine_predicted_unvalidated"},"labels":[],"label_agreement":null},{"id":"W2790353594","doi":"10.22323/1.020.0211","title":"The determination of decay constants f_D_s and f_D in three-flavor lattice QCD","year":2005,"lang":"en","type":"article","venue":"Proceedings of XXIIIrd International Symposium on Lattice Field Theory — PoS(LAT2005)","topic":"Quantum Chromodynamics and Particle Interactions","field":"Physics and Astronomy","cited_by":0,"is_retracted":false,"has_abstract":true,"routes":{"ca_aff":true,"ca_fund":false,"ca_venue":false,"about_ca":false},"ca_institutions":"Simon Fraser University","funders":"","keywords":"Physics; Extrapolation; Lattice QCD; Chiral perturbation theory; Lattice (music); Lattice constant; Particle physics; Quark; Quantum chromodynamics; Meson; Lattice field theory; Systematic error; Flavor; Nuclear physics; Quantum mechanics; Mathematics; Statistics; Chemistry","authors":[{"name":"James N. Simone","is_ca":false},{"name":"Christopher Aubin","is_ca":false},{"name":"C. Bérnard","is_ca":false},{"name":"Massimo Di Pierro","is_ca":false},{"name":"E. D. Freeland","is_ca":false},{"name":"Steven Gottlieb","is_ca":false},{"name":"Urs M. Heller","is_ca":false},{"name":"J. E. Hetrick","is_ca":false},{"name":"A. X. El-Khadra","is_ca":false},{"name":"Andreas S. Kronfeld","is_ca":false},{"name":"L. Levkova","is_ca":false},{"name":"Paul B. Mackenzie","is_ca":false},{"name":"D. Menscher","is_ca":false},{"name":"F. Maresca","is_ca":false},{"name":"M. Nobes","is_ca":false},{"name":"M. Okamoto","is_ca":false},{"name":"Dru B. Renner","is_ca":false},{"name":"R. Sugar","is_ca":false},{"name":"D. Toussaint","is_ca":false},{"name":"Howard D. Trottier","is_ca":true}],"retraction":null,"screen_n_in":null,"score":{"opus":0.007552080979850049,"gpt":0.2658821968327652,"spread":0.2583301158529152,"validation_status":"score_only:v0-immature-baseline"},"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.001986679,0.0004769246,0.0004922515,0.001568214,0.001842051,0.00113687,0.001410819,0.0009640465,0.0006136207],"category_scores_gemma":[0.004807113,0.000447276,0.0005521533,0.001407231,0.001174608,0.0007068645,0.0005389677,0.001009898,0.00008600524],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.002414491,"about_ca_system_score_gemma":0.001941106,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.01805028,"about_ca_topic_score_gemma":0.01349698,"domain_scores_codex":[0.9994764,0.000196109,0.00002082216,0.00005488635,0.0001436528,0.0001081142],"domain_scores_gemma":[0.9969904,0.001865413,0.0003219199,0.0002155177,0.0003869533,0.0002196798],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"simulation_or_modeling","study_design_gemma":"simulation_or_modeling","study_design_scores_codex":[0.0009271854,0.0006107583,0.06533878,0.0002454634,0.0001567341,0.0008353658,0.0008827746,0.689922,0.06150011,0.1488757,0.001121518,0.02958358],"study_design_scores_gemma":[0.0001382541,0.00004913278,0.004127895,0.00002875455,0.00001644247,0.0001314458,0.0001083086,0.9545318,0.02017982,0.02025754,0.0003618368,0.00006872789],"study_design_candidate":"simulation_or_modeling","study_design_consensus":"simulation_or_modeling","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9828934,0.0001941096,0.01400369,0.0001986164,0.00001691501,0.00001150677,0.0000814527,0.0002118216,0.002388567],"genre_scores_gemma":[0.9937039,0.00004246107,0.006097998,0.00001992655,0.00000234008,0.0000088385,0.00003176837,0.00001314166,0.0000795572],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.01805028,"threshold_uncertainty_score":0.03589046,"prediction_status":"machine_predicted_unvalidated"},"labels":[],"label_agreement":null}]}