{"id":"W2409302856","doi":"10.1007/jhep03(2015)092","title":"Measurement of dijet production in diffractive deep-inelastic ep scattering at HERA","year":2015,"lang":"en","type":"article","venue":"Journal of High Energy Physics","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":21,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of Toronto","funders":"Deutsches Elektronen-Synchrotron; Science and Technology Facilities Council; Fonds De La Recherche Scientifique - FNRS; Vlaamse regering; Vedecká Grantová Agentúra MŠVVaŠ SR a SAV; Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung; Autoritatea Natională pentru Cercetare Stiintifică; Fonds Wetenschappelijk Onderzoek; Bundesministerium für Bildung und Forschung; Russian Foundation for Basic Research; Consejo Nacional de Ciencia y Tecnología; National Science Foundation","keywords":"HERA; Physics; Deep inelastic scattering; Parton; Particle physics; Nuclear physics; Quantum chromodynamics; Scattering; Coupling constant; Photon; Inelastic scattering; Optics","routes":{"ca_aff":true,"ca_fund":false,"ca_venue":false,"about_ca":false,"invisible_to_affiliation_only":false},"retraction":null,"screen":null,"direct_labels":[],"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0006857723,0.0008757334,0.0005488921,0.00229182,0.0005493935,0.0007123747,0.0006496583,0.0005673081,0.001855585],"category_scores_gemma":[0.001187704,0.0004921139,0.0002935421,0.001804185,0.0004493765,0.0004818607,0.000973292,0.0005641513,0.0002637581],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0008057926,"about_ca_system_score_gemma":0.0002408143,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.001292521,"about_ca_topic_score_gemma":0.001027429,"domain_scores_codex":[0.9994568,0.0001223254,0.0000203973,0.0001302169,0.0001846524,0.00008563754],"domain_scores_gemma":[0.9991283,0.0003833373,0.0001555114,0.0001282195,0.00009097971,0.0001136136],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"bench_or_experimental","study_design_gemma":"observational","study_design_scores_codex":[0.00338716,0.0004172075,0.08550686,0.0005737419,0.0005595529,0.002883944,0.0005959921,0.02127735,0.8529556,0.00708404,0.0006011748,0.02415734],"study_design_scores_gemma":[0.0003073838,0.001318609,0.2633015,0.00005488694,0.0002153761,0.003897724,0.000379448,0.05988963,0.6611525,0.004938157,0.004351988,0.000192816],"study_design_candidate":"observational","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9930925,0.0004555273,0.003123003,0.0000626228,0.000007303156,0.00001457056,0.0009463849,0.0001148052,0.002183208],"genre_scores_gemma":[0.9979957,0.0001577017,0.0008368088,0.00001850474,0.000003834894,0.00001041452,0.0004553093,0.00001147504,0.0005102128],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.00229182,"threshold_uncertainty_score":0.006207526,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02198090513461947,"score_gpt":0.2442678250281862,"score_spread":0.2222869198935667,"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."}}