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The Asymptotic 3-Loop Heavy Flavor Corrections to the Charged Current Structure Functions FLW+−W−(x,Q2)F_L^{W^+-W^-}(x,Q^2) and F2W+−W−(x,Q2)F_2^{W^+-W^-}(x,Q^2)

Published 20 Sep 2016 in hep-ph and hep-ex | (1609.06255v1)

Abstract: We calculate the massive Wilson coefficients for the heavy flavor contributions to the non-singlet charged current deep-inelastic scattering structure functions FL<sup>W<sup>+(x,Q<sup>2)−FL<sup>W<sup>−(x,Q<sup>2)F_L<sup>{W<sup>+}(x,Q<sup>2)-F_L<sup>{W<sup>-}(x,Q<sup>2) and F2<sup>W<sup>+(x,Q<sup>2)−F2<sup>W<sup>−(x,Q<sup>2)F_2<sup>{W<sup>+}(x,Q<sup>2)-F_2<sup>{W<sup>-}(x,Q<sup>2) in the asymptotic region Q<sup>2</sup>≫m<sup>2Q<sup>2</sup> \gg m<sup>2 to 3-loop order in Quantum Chromodynamics (QCD) at general values of the Mellin variable NN and the momentum fraction xx. Besides the heavy quark pair production, also the single heavy flavor excitation s→cs \rightarrow c contributes. Numerical results are presented for the charm quark contributions and consequences on the unpolarized Bjorken sum rule and Adler sum rule are discussed.

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