{"meta":{"query_hash":"87bf78fc28b3","filters":{"venue":"ESAIM. Mathematical modelling and numerical analysis"},"cohort_total":8,"direct_labels_cover":0,"predictions_cover":8,"exported":8,"export_cap":100000,"truncated":false,"label_status":"direct model label, unvalidated","prediction_status":"machine_predicted_unvalidated (Codex and Gemma teacher distillation)","score_status":"score_only:v0-immature-baseline","snapshot":{"source":"OpenAlex, pinned release, all 482 partitions","release":"2026-06-24","frame_built":"2026-07-12"},"permalink":"https://metacan.xera.ac/q/87bf78fc28b3","api":"https://metacan.xera.ac/api/v1/cohort?venue=ESAIM.+Mathematical+modelling+and+numerical+analysis"},"results":[{"id":"W4321018154","doi":"10.1051/m2an/2023016","title":"A hybridizable discontinuous Galerkin method for the fully coupled time-dependent Stokes/Darcy-transport problem","year":2023,"lang":"en","type":"article","venue":"ESAIM. Mathematical modelling and numerical analysis","topic":"Advanced Numerical Methods in Computational Mathematics","field":"Engineering","cited_by":5,"is_retracted":false,"has_abstract":true,"route_ca_aff":false,"route_ca_fund":true,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"","funders":"Natural Sciences and Engineering Research Council of Canada","keywords":"Discontinuous Galerkin method; Convection–diffusion equation; Stokes flow; Mathematics; Mathematical analysis; Discretization; Darcy's law; Applied mathematics; Flow (mathematics); Physics; Porous medium; Finite element method; Geometry","score_opus":0.023415152630379577,"score_gpt":0.28719427506931905,"score_spread":0.2637791224389395,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W4321018154","genre_codex":"methods","genre_gemma":"methods","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"methods","genre_consensus":"methods","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.0016761106,0.00025284008,0.99595743,0.0004147168,0.000053492608,0.00058966386,0.000046011744,0.00068164425,0.0003281127],"genre_scores_gemma":[0.07418136,0.00009453862,0.92414904,0.00005791916,0.0000940533,0.0003333372,0.000038676684,0.000101579324,0.00094951154],"study_design_codex":"simulation_or_modeling","study_design_gemma":"simulation_or_modeling","domain_scores_codex":[0.9973379,0.000095793046,0.0008585118,0.0005111002,0.00057033985,0.0006264036],"domain_scores_gemma":[0.9939837,0.005110055,0.00012531262,0.0004325465,0.00011912569,0.00022929802],"candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.0013776686,0.0004018192,0.001013475,0.00024152019,0.00028290684,0.0001044671,0.00034371496,0.000110736706,0.00010439871],"category_scores_gemma":[0.00018559414,0.0002826995,0.0004615448,0.0016744048,0.00010393044,0.00014814819,0.00007027369,0.00032605734,0.00008871739],"study_design_candidate":"simulation_or_modeling","study_design_consensus":"simulation_or_modeling","about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.000024886995,0.0000705968,0.000009771056,0.00026859035,0.00096029235,0.000006400724,0.00025245766,0.9898818,0.0001399314,0.0045697177,0.00007558939,0.003739953],"study_design_scores_gemma":[0.0002048103,0.000037858645,0.00000644289,0.00003445294,0.0010998147,0.000007656591,0.0000691032,0.7905316,0.00008161636,0.20735389,0.0002744599,0.00029834002],"about_ca_topic_score_codex":0.000011783422,"about_ca_topic_score_gemma":6.779039e-7,"teacher_disagreement_score":0.20278417,"about_ca_system_score_codex":0.000052760184,"about_ca_system_score_gemma":0.000017532535,"threshold_uncertainty_score":0.9999625},"labels":[],"label_agreement":null},{"id":"W4378802446","doi":"10.1051/m2an/2023038","title":"Fully discrete Schwarz waveform relaxation analysis for the heat equation on a finite spatial domain","year":2023,"lang":"en","type":"article","venue":"ESAIM. Mathematical modelling and numerical analysis","topic":"Numerical methods for differential equations","field":"Mathematics","cited_by":2,"is_retracted":false,"has_abstract":true,"route_ca_aff":true,"route_ca_fund":true,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"Memorial University of Newfoundland","funders":"Natural Sciences and Engineering Research Council of Canada","keywords":"Schwarz alternating method; Partial differential equation; Mathematics; Bounded function; Waveform; Heat equation; Mathematical analysis; Discrete time and continuous time; Norm (philosophy); Additive Schwarz method; Relaxation (psychology); Integrator; Applied mathematics; Domain decomposition methods; Finite element method; Computer science","score_opus":0.10012197886356536,"score_gpt":0.3416166963838536,"score_spread":0.24149471752028825,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W4378802446","genre_codex":"methods","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"methods","genre_consensus":null,"domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.018593762,0.000025305166,0.9775972,0.0025540655,0.00006135482,0.00063945755,0.000066734196,0.00026519815,0.00019694379],"genre_scores_gemma":[0.7097968,0.000035230827,0.28890932,0.00009289234,0.000137912,0.0003324501,0.00018114691,0.000053983273,0.00046030185],"study_design_codex":"simulation_or_modeling","study_design_gemma":"simulation_or_modeling","domain_scores_codex":[0.99645376,0.00031396214,0.0010665406,0.00070514355,0.0008617177,0.00059889926],"domain_scores_gemma":[0.987885,0.0106497975,0.00030397557,0.0007378251,0.0001714797,0.0002518977],"candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.0018817784,0.00041173876,0.0011300431,0.00084569294,0.00071402965,0.00019063188,0.00030373695,0.00019625456,0.00017883592],"category_scores_gemma":[0.002037375,0.00026213707,0.0011983564,0.0050201775,0.00015330703,0.00013239477,0.000105700536,0.00033976955,0.00008392607],"study_design_candidate":"simulation_or_modeling","study_design_consensus":"simulation_or_modeling","about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.00031266405,0.0004526206,0.000281798,0.00020179024,0.009351796,0.0000037177076,0.0020407876,0.72182655,0.00006589633,0.25280344,0.000060837534,0.01259807],"study_design_scores_gemma":[0.00020007162,0.00009088448,0.000096471405,0.000016323831,0.0050295275,3.2797618e-7,0.00012073966,0.5402922,0.000029000325,0.45388597,0.000051555584,0.00018696234],"about_ca_topic_score_codex":0.00014222582,"about_ca_topic_score_gemma":0.000022219532,"teacher_disagreement_score":0.691203,"about_ca_system_score_codex":0.00008728753,"about_ca_system_score_gemma":0.000023028377,"threshold_uncertainty_score":0.9999831},"labels":[],"label_agreement":null},{"id":"W4385648137","doi":"10.1051/m2an/2023052","title":"Numerical analysis of finite element methods for the cardiac extracellular-membrane-intracellular model: Steklov–Poincaré operator and spatial error estimates","year":2023,"lang":"en","type":"article","venue":"ESAIM. Mathematical modelling and numerical analysis","topic":"Elasticity and Material Modeling","field":"Engineering","cited_by":3,"is_retracted":false,"has_abstract":true,"route_ca_aff":true,"route_ca_fund":true,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"University of Ottawa","funders":"Division of Mathematical Sciences; National Eye Institute; Natural Sciences and Engineering Research Council of Canada","keywords":"Finite element method; Ode; Discretization; Operator (biology); Applied mathematics; Mathematics; Nonlinear system; Mathematical analysis; Convergence (economics); Numerical analysis; Physics","score_opus":0.030830301749179317,"score_gpt":0.2915954140313322,"score_spread":0.2607651122821529,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W4385648137","genre_codex":"methods","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"methods","genre_consensus":null,"domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.060550272,0.0013834096,0.93720984,0.0001404881,0.00006775411,0.0003366507,0.00007998203,0.00021152306,0.00002004646],"genre_scores_gemma":[0.8088394,0.00043054798,0.19038181,0.00001613747,0.000050290953,0.000115514944,0.00007202729,0.000053541233,0.00004074302],"study_design_codex":"simulation_or_modeling","study_design_gemma":"simulation_or_modeling","domain_scores_codex":[0.9974542,0.000119279306,0.0009744373,0.0005371284,0.00034952688,0.00056540524],"domain_scores_gemma":[0.9968111,0.0022647406,0.00012139889,0.00042893045,0.00011754012,0.0002562901],"candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.0011870603,0.00042008705,0.0015494233,0.00047273518,0.00026368728,0.00013031495,0.00022940202,0.00018264003,0.000062420484],"category_scores_gemma":[0.00019439001,0.00031022215,0.0006696535,0.0017956363,0.00013115667,0.00009940272,0.000102465725,0.00023632841,0.0000066386838],"study_design_candidate":"simulation_or_modeling","study_design_consensus":"simulation_or_modeling","about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.000043474436,0.000053589192,0.000049476752,0.0003073626,0.0053874278,0.000001763625,0.0005978275,0.9860957,0.0040052077,0.0014969971,0.000005731462,0.0019553935],"study_design_scores_gemma":[0.00020123456,0.00004955509,0.000009176282,0.0000336177,0.013385411,5.8158065e-7,0.00011115687,0.9777885,0.0038368287,0.0041842894,0.000045765923,0.00035387382],"about_ca_topic_score_codex":0.00014207007,"about_ca_topic_score_gemma":0.000003553202,"teacher_disagreement_score":0.7482891,"about_ca_system_score_codex":0.000028903285,"about_ca_system_score_gemma":0.000016789736,"threshold_uncertainty_score":0.999935},"labels":[],"label_agreement":null},{"id":"W4387834348","doi":"10.1051/m2an/2023086","title":"A strongly conservative hybridizable discontinuous Galerkin method for the coupled time-dependent Navier–Stokes and Darcy problem","year":2023,"lang":"en","type":"article","venue":"ESAIM. Mathematical modelling and numerical analysis","topic":"Numerical methods for differential equations","field":"Mathematics","cited_by":10,"is_retracted":false,"has_abstract":true,"route_ca_aff":false,"route_ca_fund":true,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"","funders":"Natural Sciences and Engineering Research Council of Canada; National Science Foundation","keywords":"Uniqueness; Discontinuous Galerkin method; Mathematics; Darcy's law; Backward Euler method; Time stepping; A priori and a posteriori; Euler's formula; Applied mathematics; Mathematical analysis; Stokes problem; Darcy–Weisbach equation; Euler equations; Finite element method; Porous medium; Physics; Discretization","score_opus":0.06645919325499679,"score_gpt":0.3502542329658449,"score_spread":0.28379503971084813,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W4387834348","genre_codex":"methods","genre_gemma":"methods","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"methods","genre_consensus":"methods","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.013089944,0.00016998511,0.98359185,0.0017287922,0.000027027907,0.00093450514,0.0000808128,0.00023733295,0.00013972154],"genre_scores_gemma":[0.067885235,0.0000781253,0.92823154,0.00006757323,0.000070510076,0.0004989347,0.000041996747,0.0000797492,0.003046328],"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"simulation_or_modeling","domain_scores_codex":[0.99676347,0.00040656776,0.000908646,0.00071227894,0.00056260993,0.0006464324],"domain_scores_gemma":[0.9872578,0.011460863,0.00031599076,0.0004975686,0.00018412223,0.00028367064],"candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.0021910681,0.0004218499,0.0012920022,0.00024409422,0.00057693745,0.0002717489,0.00029302412,0.00012594328,0.00014946864],"category_scores_gemma":[0.0010833266,0.0002726681,0.00045052654,0.0014021518,0.0002512764,0.00017167104,0.00020215524,0.00033214316,0.00003467293],"study_design_candidate":"theoretical_or_conceptual","study_design_consensus":null,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.0010851995,0.003263035,0.0007393885,0.0032000612,0.025919536,0.00005544504,0.011217247,0.20972511,0.0033305034,0.6612323,0.0014260035,0.078806184],"study_design_scores_gemma":[0.000288504,0.00006842121,0.00001112861,0.000034656678,0.0021614188,0.000004208272,0.00022071628,0.57959944,0.000057906676,0.4172614,0.00008409939,0.00020810151],"about_ca_topic_score_codex":0.0001244351,"about_ca_topic_score_gemma":0.000005810071,"teacher_disagreement_score":0.36987433,"about_ca_system_score_codex":0.000039171242,"about_ca_system_score_gemma":0.000034530185,"threshold_uncertainty_score":0.9999725},"labels":[],"label_agreement":null},{"id":"W4399394642","doi":"10.1051/m2an/2024045","title":"A hybridizable discontinuous Galerkin method for the coupled Navier–Stokes/Biot problem","year":2024,"lang":"en","type":"article","venue":"ESAIM. Mathematical modelling and numerical analysis","topic":"Advanced Numerical Methods in Computational Mathematics","field":"Engineering","cited_by":4,"is_retracted":false,"has_abstract":true,"route_ca_aff":false,"route_ca_fund":true,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"","funders":"Natural Sciences and Engineering Research Council of Canada; National Science Foundation","keywords":"Discontinuous Galerkin method; Biot number; A priori and a posteriori; Mathematics; Stability (learning theory); Galerkin method; Pointwise; Poromechanics; Mathematical analysis; Applied mathematics; Finite element method; Computer science; Physics; Porous medium; Mechanics","score_opus":0.026904669727186952,"score_gpt":0.30693799596371896,"score_spread":0.280033326236532,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W4399394642","genre_codex":"methods","genre_gemma":"methods","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"methods","genre_consensus":"methods","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.00029289414,0.0032866965,0.9942013,0.0005603733,0.00010862666,0.00046687186,0.000028507653,0.0005271308,0.00052759424],"genre_scores_gemma":[0.08836332,0.00015447136,0.9106691,0.000060955666,0.00013352114,0.00024512658,0.0000125841,0.00008477487,0.00027613473],"study_design_codex":"simulation_or_modeling","study_design_gemma":"simulation_or_modeling","domain_scores_codex":[0.99779075,0.00008351109,0.00074491155,0.00050083915,0.00039286795,0.00048711005],"domain_scores_gemma":[0.99265844,0.006649141,0.00006584629,0.00035453142,0.00008157927,0.00019046894],"candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.00097417977,0.00037793096,0.0008523268,0.00018828333,0.00021514176,0.00023558969,0.00026917143,0.00010572164,0.00009381444],"category_scores_gemma":[0.00018326596,0.00024727694,0.0004949379,0.0013627547,0.000108457876,0.00013033634,0.000068385074,0.00038169717,0.00003427917],"study_design_candidate":"simulation_or_modeling","study_design_consensus":"simulation_or_modeling","about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.000011859436,0.000055960492,0.0000015209677,0.00064101873,0.0012561751,0.0000051893903,0.0002917315,0.93488896,0.00007398601,0.046242613,0.00011651407,0.01641449],"study_design_scores_gemma":[0.00007996388,0.000026698464,5.8071646e-7,0.00007757205,0.0011654131,0.000012712044,0.000044395827,0.66479874,0.0000620039,0.3322901,0.0012137862,0.00022801018],"about_ca_topic_score_codex":0.000009464513,"about_ca_topic_score_gemma":3.2999333e-7,"teacher_disagreement_score":0.2860475,"about_ca_system_score_codex":0.00006109075,"about_ca_system_score_gemma":0.00001678971,"threshold_uncertainty_score":0.999998},"labels":[],"label_agreement":null},{"id":"W4403823555","doi":"10.1051/m2an/2024075","title":"A hybrid finite element method for moving-habitat models in two spatial dimensions","year":2024,"lang":"en","type":"article","venue":"ESAIM. Mathematical modelling and numerical analysis","topic":"Evacuation and Crowd Dynamics","field":"Engineering","cited_by":0,"is_retracted":false,"has_abstract":true,"route_ca_aff":true,"route_ca_fund":true,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"University of Ottawa","funders":"Natural Sciences and Engineering Research Council of Canada","keywords":"Finite element method; Element (criminal law); Habitat; Geography; Computer science; Structural engineering; Engineering; Ecology; Political science; Biology","score_opus":0.021674951705371884,"score_gpt":0.2914441115052963,"score_spread":0.26976915979992444,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W4403823555","genre_codex":"methods","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"methods","genre_consensus":null,"domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.00876252,0.00044624077,0.9897341,0.0002181,0.0000426331,0.0001767211,0.000032689928,0.00021629309,0.00037068786],"genre_scores_gemma":[0.72569937,0.00006190456,0.27396882,0.000044750064,0.000030258581,0.00006905981,0.00003104722,0.000030209621,0.000064589876],"study_design_codex":"simulation_or_modeling","study_design_gemma":"simulation_or_modeling","domain_scores_codex":[0.9985693,0.000041819017,0.0005151611,0.0003397607,0.00021904704,0.00031489567],"domain_scores_gemma":[0.9987445,0.000861768,0.000022642998,0.00018655113,0.00003569154,0.000148849],"candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.00044904242,0.00021585856,0.0004919571,0.00033540954,0.000063148305,0.000101851016,0.000085894724,0.0000462458,0.000063166204],"category_scores_gemma":[0.000038741047,0.00018413551,0.0002726231,0.0005431159,0.000022387672,0.00010587269,0.000033866298,0.00019993946,0.00001824187],"study_design_candidate":"simulation_or_modeling","study_design_consensus":"simulation_or_modeling","about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.000007806397,0.000047407022,0.000009970079,0.00014086536,0.00032871947,0.0000056884155,0.00028565366,0.96554863,0.000025048856,0.030390533,0.000023023127,0.0031866506],"study_design_scores_gemma":[0.00015183161,0.000016792495,0.0000011125603,0.00004438028,0.00047309784,0.0000017823207,0.000028168375,0.7841611,0.000035838082,0.21485177,0.000055882716,0.00017824445],"about_ca_topic_score_codex":0.000052472842,"about_ca_topic_score_gemma":0.000022515194,"teacher_disagreement_score":0.7169368,"about_ca_system_score_codex":0.00005700303,"about_ca_system_score_gemma":0.0000123896,"threshold_uncertainty_score":0.75088286},"labels":[],"label_agreement":null},{"id":"W4413977537","doi":"10.1051/m2an/2025073","title":"Bounding escape rates and approximating quasi-stationary distributions of Brownian dynamics","year":2025,"lang":"en","type":"article","venue":"ESAIM. Mathematical modelling and numerical analysis","topic":"Diffusion and Search Dynamics","field":"Biochemistry, Genetics and Molecular Biology","cited_by":0,"is_retracted":false,"has_abstract":true,"route_ca_aff":false,"route_ca_fund":true,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"","funders":"Fonds de recherche du Québec – Nature et technologies","keywords":"Bounding overwatch; Statistical physics; Mathematics; Dynamics (music); Brownian motion; Physics; Computer science; Statistics","score_opus":0.011310329936893614,"score_gpt":0.2790342537354422,"score_spread":0.2677239237985486,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W4413977537","genre_codex":"methods","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"empirical","genre_consensus":null,"domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.30117798,0.00016667166,0.6978474,0.0002365057,0.0000068076624,0.000052707303,0.000027153457,0.000008022636,0.00047670174],"genre_scores_gemma":[0.94983774,0.00013572501,0.049415965,0.000041043157,0.0000097674465,0.000008718915,0.00021538693,0.0000070710093,0.00032855614],"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"simulation_or_modeling","domain_scores_codex":[0.9989886,0.000059058802,0.0003638734,0.00027669535,0.00013172624,0.00017998961],"domain_scores_gemma":[0.9994416,0.00012716369,0.000080175574,0.00017340317,0.00007851086,0.000099151],"candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.00026912856,0.0001277382,0.00032392,0.0001241403,0.00016177997,0.00004739279,0.00008459253,0.00008892514,0.0000145956965],"category_scores_gemma":[0.00016205122,0.00010926717,0.00012561819,0.0004565725,0.0001518251,0.00000624827,0.00010922942,0.000095560994,8.4798813e-7],"study_design_candidate":"simulation_or_modeling","study_design_consensus":null,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.00031929393,0.0024113986,0.025650997,0.0016319291,0.0044830544,0.000008372144,0.0010130767,0.05348505,0.013911905,0.8658672,0.00013376784,0.031083945],"study_design_scores_gemma":[0.00014202869,0.00004807307,0.00016518307,0.00003101951,0.0002792183,0.0000017628022,0.00024129973,0.97024447,0.00025385217,0.028438177,0.000045761517,0.00010916509],"about_ca_topic_score_codex":0.000019942538,"about_ca_topic_score_gemma":0.000005304655,"teacher_disagreement_score":0.91675943,"about_ca_system_score_codex":0.000012595241,"about_ca_system_score_gemma":0.00002469159,"threshold_uncertainty_score":0.44557858},"labels":[],"label_agreement":null},{"id":"W4414454059","doi":"10.1051/m2an/2025080","title":"Convergence of a semi-explicit scheme for a one dimensional periodic nonlocal eikonal equation modeling dislocation dynamics","year":2025,"lang":"en","type":"article","venue":"ESAIM. Mathematical modelling and numerical analysis","topic":"Numerical methods in inverse problems","field":"Mathematics","cited_by":1,"is_retracted":false,"has_abstract":true,"route_ca_aff":true,"route_ca_fund":false,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"Université de Montréal","funders":"","keywords":"Eikonal equation; Convergence (economics); Scheme (mathematics); Entropy (arrow of time); Dislocation; Numerical analysis; Set (abstract data type)","score_opus":0.08840718710176779,"score_gpt":0.3368771629489844,"score_spread":0.2484699758472166,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W4414454059","genre_codex":"methods","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"methods","genre_consensus":null,"domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.04342209,0.00011391825,0.955161,0.0005280523,0.000048265225,0.0004296904,0.00003010838,0.00008205301,0.00018481704],"genre_scores_gemma":[0.5013,0.00001437115,0.4983845,0.000050718943,0.000018220115,0.00009185328,0.000028397648,0.000018747867,0.00009319448],"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"simulation_or_modeling","domain_scores_codex":[0.9969095,0.00015382783,0.0012733215,0.0006477512,0.00059366954,0.00042191148],"domain_scores_gemma":[0.99616814,0.0024855076,0.00031753985,0.0004502199,0.0003968347,0.00018175034],"candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.0011740263,0.00033629022,0.0011786778,0.00038180113,0.00022995567,0.00004878429,0.00024840597,0.00022285857,0.00010591617],"category_scores_gemma":[0.0011085422,0.0003018268,0.0004875529,0.001435863,0.00017346618,0.00013046621,0.00014487804,0.00028665684,0.000006256773],"study_design_candidate":"theoretical_or_conceptual","study_design_consensus":null,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.00021731276,0.00096377893,0.00023566518,0.0012404735,0.0016265305,7.042217e-7,0.00065630366,0.2782139,0.00044576533,0.71372956,0.000016299253,0.0026537206],"study_design_scores_gemma":[0.0002331962,0.0000433096,8.97081e-7,0.00012912015,0.0010042497,7.241479e-7,0.00008833895,0.56217563,0.0001556118,0.4360002,0.0000022845106,0.00016645342],"about_ca_topic_score_codex":0.00006092975,"about_ca_topic_score_gemma":0.0000021601381,"teacher_disagreement_score":0.4578779,"about_ca_system_score_codex":0.000136084,"about_ca_system_score_gemma":0.00007666083,"threshold_uncertainty_score":0.9999434},"labels":[],"label_agreement":null}]}