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Functional and structural properties of gum arabic complexes with casein and hydrolyzed casein achieved by Maillard reaction
Identification of male sterile (T, S) of fertility (N) cytoplasm by PCR-based molecular markers to access maintainer lines in onion
Identification of male sterile (T, S) of fertility (N) cytoplasm by PCR-based molecular markers to access maintainer lines in onion
Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton-proton collisions at $$\sqrt{s} = 13\,\text {Te}\text {V} $$
Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton-proton collisions at $$\sqrt{s} = 13\,\text {Te}\text {V} $$
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
Day 7 Embryos Change the Proteomics and Exosomal Micro-RNAs Content of Bovine Uterine Fluid: Involvement of Innate Immune Functions
Pollination system and deficit irrigation affect flavonolignan components of sylimarin, oil, and productivity of milk thistle
Magnetic chitosan-functionalized cobalt-NHC: Synthesis, characterization and catalytic activity toward Suzuki and Sonogashira cross-coupling reactions of aryl chlorides
Bending analysis of functionally graded sandwich plates using the refined finite strip method
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