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The Polarized Three-Loop Anomalous Dimensions from On-Shell Massive Operator Matrix Elements

High Energy Physics - Phenomenology 2019-09-25 v1 High Energy Physics - Theory

Abstract

We calculate all contributions TF\propto T_F to the polarized three-loop anomalous dimensions in the M-scheme using massive operator matrix elements and compare to results in the literature. This includes the complete anomalous dimensions γqq(2),PS\gamma_{qq}^{(2),\rm PS} and γqg(2)\gamma_{qg}^{(2)}. We also obtain the complete two-loop polarized anomalous dimensions in an independent calculation. While for most of the anomalous dimensions the usual direct computation methods in Mellin NN-space can be applied since all recurrences factorize at first order, this is not the case for γqg(2)\gamma_{qg}^{(2)}. Due to the necessity of deeper expansions of the master integrals in the dimensional parameter ε=D4\varepsilon = D-4, we had to use the method of arbitrary high moments to eliminate elliptic contributions in intermediate steps. 4000 moments were generated to determine this anomalous dimension and 2640 moments turned out to be sufficient. As an aside, we also recalculate the contributions TF\propto T_F to the three-loop QCD β\beta-function.

Keywords

Cite

@article{arxiv.1908.03779,
  title  = {The Polarized Three-Loop Anomalous Dimensions from On-Shell Massive Operator Matrix Elements},
  author = {A. Behring and J. Blümlein and A. De Freitas and A. Goedicke and S. Klein and A. von Manteuffel and C. Schneider and K. Schönwald},
  journal= {arXiv preprint arXiv:1908.03779},
  year   = {2019}
}

Comments

40 pages Latex, 2 Figures

R2 v1 2026-06-23T10:44:24.805Z