Third-order QCD corrections to the charged-current structure function \(F_{3}\)
From MaRDI portal
Publication:993162
DOI10.1016/j.nuclphysb.2009.01.001zbMath1194.81271arXiv0812.4168OpenAlexW2103167339MaRDI QIDQ993162
A. Vogt, J. A. M. Vermaseren, S. Moch
Publication date: 10 September 2010
Published in: Nuclear Physics. B (Search for Journal in Brave)
Full work available at URL: https://arxiv.org/abs/0812.4168
Nuclear physics (81V35) Strong interaction, including quantum chromodynamics (81V05) Perturbative methods of renormalization applied to problems in quantum field theory (81T15) Inelastic and multichannel quantum scattering (81U35)
Related Items
The complete \(O(\alpha_s^2)\) non-singlet heavy flavor corrections to the structure functions \(g_{1, 2}^{e p}(x, Q^2)\), \(F_{1, 2, L}^{e p}(x, Q^2)\), \(F_{1, 2, 3}^{\nu(\overline{\nu})}(x, Q^2)\) and the associated sum rules, The two-loop massless off-shell QCD operator matrix elements to finite terms, 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, On Higgs-exchange DIS, physical evolution kernels and fourth-order splitting functions at large x, Four-loop splitting functions in QCD -- the quark-quark case, The five-loop beta function of Yang-Mills theory with fermions, The massless three-loop Wilson coefficients for the deep-inelastic structure functions \(F_2\), \(F_L\), \(xF_3\) and \(g_1\), \(O(\alpha_s^2)\) polarized heavy flavor corrections to deep-inelastic scattering at \(Q^2 \gg m^2\), The 3-loop non-singlet heavy flavor contributions to the structure function \(g_1(x, Q^2)\) at large momentum transfer, Three-loop anomalous dimension of the non-singlet transversity operator in QCD, On the next-to-next-to-leading order QCD corrections to heavy-quark production in deep-inelastic scattering, Four-loop non-singlet splitting functions in the planar limit and beyond, Generalized double-logarithmic large-x resummation in inclusive deep-inelastic scattering, Resummation of small-\(x\) double logarithms in QCD: semi-inclusive electron-positron annihilation, The \(\mathrm{N^3LO}\) scheme-invariant QCD evolution of the non-singlet structure functions \(F_2^{\mathrm{NS}}(x, Q^2)\) and \(g_1^{\mathrm{NS}}(x, Q^2)\), Large-\(n_{f}\) contributions to the four-loop splitting functions in QCD
Cites Work
- The three-loop splitting functions in QCD: the non-singlet case
- The three-loop splitting functions in QCD: the singlet case
- The four-loop QCD \(\beta\)-function and anomalous dimensions
- The third-order QCD corrections to deep-inelastic scattering by photon exchange
- Higher-order corrections in threshold resummation
- Multiple polylogarithms, cyclotomy and modular complexes
- Automatic Feynman graph generation
- Differences between charged-current coefficient functions
- HARMONIC SUMS, MELLIN TRANSFORMS AND INTEGRALS
- HARMONIC POLYLOGARITHMS
- Special values of multiple polylogarithms
- Non-singlet structure functions beyond the next-to-next-to-leading order
