Report/Internal Report PUBDB-2015-02312

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On $\gamma_5$ in higher-order QCD calculations and the NNLO evolution of the polarized valence distribution

 ;  ;

2015

11 p. ()  GO

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Report No.: DESY-15-061; LTH-1042; NIKHEF-15-018; arXiv:1506.04517

Abstract: We discuss the prescription for the Dirac matrix gamma_5 in dimensional regularization used in most second- and third-order QCD calculations of collider cross sections. We provide an alternative implementation of this approach that avoids the use of an explicit form of gamma_5 and of its (anti-) commutation relations in the most important case of no more than one gamma_5 in each fermion trace. This treatment is checked by computing the third-order corrections to the structure functions F_2 and g_1 in charged-current deep-inelastic scattering with axial-vector couplings to the W-bosons. We derive the so far unknown third-order helicity-difference splitting function Delta P_ns^(2)s that contributes to the next-to-next-to-leading order (NNLO) evolution of the polarized valence quark distribution of the nucleon. This function is negligible at momentum fractions x >~ 0.3 but relevant at x << 1.

Keyword(s): regularization: dimensional ; coupling: axial-vector ; higher-order: 2 ; quark: valence ; quantum chromodynamics ; deep inelastic scattering ; commutation relations ; structure function ; splitting function ; charged current ; nucleon


Contributing Institute(s):
  1. Theorie (ZEU-THEO)
Research Program(s):
  1. 611 - Fundamental Particles and Forces (POF3-611) (POF3-611)
  2. HEPGAME - Solving High Energy Physics Equations using Monte Carlo Gaming Techniques (320651) (320651)
Experiment(s):
  1. No specific instrument

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On ${\gamma }_{5}$ in higher-order QCD calculations and the NNLO evolution of the polarized valence distribution
Physics letters / B 748, 432 - 438 () [10.1016/j.physletb.2015.07.027]  GO OpenAccess  Download fulltext Files  Download fulltextFulltext by arXiv.org BibTeX | EndNote: XML, Text | RIS


 Record created 2015-06-22, last modified 2021-11-10


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