{"id":"W2957090143","doi":"10.1103/physrevlett.123.022501","title":"Measurements of Nonsinglet Moments of the Nucleon Structure Functions and Comparison to Predictions from Lattice QCD for <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mi>Q</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mo>=</mml:mo><mml:mn>4</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:msup><mml:mrow><mml:mi>GeV</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>","year":2019,"lang":"lv","type":"article","venue":"Physical Review Letters","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":4,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of Winnipeg; University of Regina","funders":"Nuclear Physics; Natural Sciences and Engineering Research Council of Canada; U.S. Department of Energy; Office of Science; National Science Foundation","keywords":"Physics; Nucleon; Particle physics; Deuterium; Lattice QCD; Quantum chromodynamics; Pion; Quark; Proton; Nuclear physics; Lattice (music)","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":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0006580098,0.0006901109,0.0002931712,0.001166337,0.0003007035,0.0005584687,0.0006615335,0.0006157951,0.002812217],"category_scores_gemma":[0.001298266,0.0005205942,0.0003213894,0.001187223,0.0003789528,0.0008370297,0.000527533,0.000747417,0.0005928676],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0006161242,"about_ca_system_score_gemma":0.0001422682,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.001512956,"about_ca_topic_score_gemma":0.003712875,"domain_scores_codex":[0.9996148,0.00005147381,0.00001402708,0.0001109935,0.0001458527,0.00006279014],"domain_scores_gemma":[0.9992213,0.000344935,0.00015436,0.0001729982,0.00006549941,0.00004083771],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"bench_or_experimental","study_design_gemma":"simulation_or_modeling","study_design_scores_codex":[0.004882975,0.0004230918,0.08403074,0.0007800238,0.0004967324,0.001213107,0.001117796,0.04986133,0.710723,0.03668569,0.005529818,0.1042557],"study_design_scores_gemma":[0.0002218457,0.0003975905,0.2189392,0.00005624316,0.0001161113,0.0007283736,0.0001819649,0.1535336,0.6063547,0.01017147,0.009101319,0.0001976102],"study_design_candidate":"simulation_or_modeling","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9284143,0.0009660238,0.04573655,0.0002410924,0.00004819003,0.00005654924,0.007067767,0.001241263,0.01622828],"genre_scores_gemma":[0.9865754,0.0002795162,0.009783862,0.00001917864,0.00001959454,0.00002345772,0.001853778,0.0001041561,0.001341011],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.002812217,"threshold_uncertainty_score":0.009407759,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02183618210933845,"score_gpt":0.2603290165034655,"score_spread":0.2384928343941271,"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."}}