Differences between charged-current coefficient functions

DOI10.1016/j.nuclphysb.2007.09.022zbMath1151.81406arXiv0708.3731OpenAlexW2029508602MaRDI QIDQ2461149

S. Moch, A. Vogt, Mikhail Rogal

Publication date: 26 November 2007

Published in: Nuclear Physics. B (Search for Journal in Brave)

Full work available at URL: https://arxiv.org/abs/0708.3731

zbMATH Keywords

quantum chromodynamicsdeep-inelastic scatteringprecision perturbative corrections

Mathematics Subject Classification ID

Strong interaction, including quantum chromodynamics (81V05)

Related Items (6)

On \(\gamma_5\) in higher-order QCD calculations and the NNLO evolution of the polarized valence distribution ⋮ The three-loop splitting functions in QCD: the helicity-dependent case ⋮ The massless three-loop Wilson coefficients for the deep-inelastic structure functions \(F_2\), \(F_L\), \(xF_3\) and \(g_1\) ⋮ The \(O({\alpha}_s^2)\) heavy quark corrections to charged current deep-inelastic scattering at large virtualities ⋮ A determination of parton distributions with faithful uncertainty estimation ⋮ Third-order QCD corrections to the charged-current structure function \(F_{3}\)

Cites Work

• The three-loop splitting functions in QCD: the non-singlet case
• The three-loop splitting functions in QCD: the singlet case
• The third-order QCD corrections to deep-inelastic scattering by photon exchange
• Higher-order corrections in threshold resummation
• HARMONIC POLYLOGARITHMS
• Non-singlet structure functions beyond the next-to-next-to-leading order
• Numerical evaluation of harmonic polylogarithms

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