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Measurement of the Wgamma Production Cross Section in Proton-Proton Collisions at sqrt s=13 TeV and Constraints on Effective Field Theory Coefficients
Measurement of the Wgamma Production Cross Section in Proton-Proton Collisions at sqrt s=13 TeV and Constraints on Effective Field Theory Coefficients
Pollination system and deficit irrigation affect flavonolignan components of sylimarin, oil, and productivity of milk thistle
Sustainable plant and microbes-mediated preparation of Fe3O4 nanoparticles and industrial application of its chitosan, starch, cellulose, and dextrin-based nanocomposites as catalysts
Parameter Estimation in Multiple Dynamic Synaptic Coupling Model Using Bayesian Point Process State-Space Modeling Framework
Parameter Estimation in Multiple Dynamic Synaptic Coupling Model Using Bayesian Point Process State-Space Modeling Framework
Insight into the effect of weld pitch on the microstructure-properties relationships of St 37/AISI 316 steels dissimilar welds processed by friction stir welding
Insight into the effect of weld pitch on the microstructure-properties relationships of St 37/AISI 316 steels dissimilar welds processed by friction stir welding
Remanufacturing the AA5052 GTAW Welds Using Friction Stir Processing
Remanufacturing the AA5052 GTAW Welds Using Friction Stir Processing
Study of Drell-Yan dimuon production in proton-lead collisions at $$ \sqrt{s_{\mathrm{NN}}} $$ = 8.16 TeV
Measurements of the differential cross sections of the production of Z + jets and gamma + jets and of Z boson emission collinear with a jet in pp collisions at $$ \sqrt{s} $$ = 13 TeV
Measurements of the differential cross sections of the production of Z + jets and gamma + jets and of Z boson emission collinear with a jet in pp collisions at $$ \sqrt{s} $$ = 13 TeV
Measurement of the Z boson differential production cross section using its invisible decay mode (Z $$ \to \nu \overline{\nu} $$) in proton-proton collisions at $$ \sqrt{s} $$ = 13 TeV
Measurement of the Z boson differential production cross section using its invisible decay mode (Z $$ \to \nu \overline{\nu} $$) in proton-proton collisions at $$ \sqrt{s} $$ = 13 TeV
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