Four-loop non-singlet splitting functions in the planar limit and beyond

A bstract We present the next-to-next-to-next-to-leading order (N 3 LO) contributions to the non-singlet splitting functions for both parton distribution and fragmentation functions in perturbative QCD. The exact expressions are derived for the terms contributing in the limit of a large number of co...

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Veröffentlicht in:The journal of high energy physics 2017-10, Vol.2017 (10), p.1-80, Article 41
Hauptverfasser: Moch, S., Ruijl, B., Ueda, T., Vermaseren, J. A. M., Vogt, A.
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Sprache:eng
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Zusammenfassung:A bstract We present the next-to-next-to-next-to-leading order (N 3 LO) contributions to the non-singlet splitting functions for both parton distribution and fragmentation functions in perturbative QCD. The exact expressions are derived for the terms contributing in the limit of a large number of colours. For the remaining contributions, approximations are provided that are sufficient for all collider-physics applications. From their threshold limits we derive analytical and high-accuracy numerical results, respectively, for all contributions to the four-loop cusp anomalous dimension for quarks, including the terms proportional to quartic Casimir operators. We briefly illustrate the numerical size of the four-loop corrections, and the remarkable renormalization-scale stability of the N 3 LO results, for the evolution of the non-singlet parton distribution and the fragmentation functions. Our results appear to provide a first point of contact of four-loop QCD calculations and the so-called wrapping corrections to anomalous dimensions in N = 4 super Yang-Mills theory.
ISSN:1029-8479
1029-8479
DOI:10.1007/JHEP10(2017)041