Abstract

We look for UV fixed points of non-abelian $SU(n_c)$ gauge theories in $4+2\epsilon$ dimensions with $n_f$ Dirac fermions in the fundamental representation, using the available five-loop $\overline{{\rm MS}}$ $\beta$-function and employing Pad\'e-Borel resummation techniques and Pad\'e approximants to the series expansion in $\epsilon$. We find evidence for a $5d$ UV-fixed point for $SU(2)$ theories with $n_f\leq 4$ and pure $SU(n_c)$ theories for $n_c\leq 4$. We also compute the anomalous dimensions $\gamma$ and $\gamma_g$ of respectively the fermion mass bilinear and the gauge kinetic term operator at the UV fixed point.

Highlights

  • Conformal Field Theories (CFTs) play a major role in theoretical physics

  • We report our results starting from the case of pure SU(2) gauge theory, our best example, and we generalize to different values of nc and nf

  • In order not to clutter the picture, the error band is shown only for the optimal approximant [2=2], which has been determined by using exact Oð1=nfÞ results for β in the large-nf limit

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Summary

Introduction

Conformal Field Theories (CFTs) play a major role in theoretical physics. In d > 4 the natural question is whether there exists a UV fixed point, i.e., an interacting CFT that when deformed by a relevant operator admits an effective description as a nonAbelian gauge theory. The existence of such a fixed point for Yang-Mills theories in d > 4 would be analogous to well-known lower-dimensional examples of perturbatively

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