Abstract

We study the gauge dependence of one-loop divergences in a general matter-coupled 6D, N=(1,0) supersymmetric gauge theory in the harmonic superspace formulation. Our analysis is based on the effective action constructed by the background superfield method, with the gauge-fixing term involving one real parameter ξ0. A manifestly gauge invariant and N=(1,0) supersymmetric procedure for calculating the one-loop effective action is developed. It yields the one-loop divergences in an explicit form and allows one to investigate their gauge dependence. As compared to the minimal gauge, ξ0=1, the divergent part of the general-gauge effective action contains a new term depending on ξ0. This term vanishes for the background superfields satisfying the classical equations of motion, so that the S-matrix divergences are gauge-independent. In the case of 6D, N=(1,1) SYM theory we demonstrate that some divergent contributions in the non-minimal gauges do not vanish off shell, as opposed to the minimal gauge.

Highlights

  • The study of quantum aspects of the higher-dimensional supersymmetric gauge field theories attracts a wide interest for a long time, mainly because of their use for the low-energy description of diverse sectors of superstring theory

  • We show that the gauge dependence of the divergences vanishes for the background superfields satisfying the classical equations of motion

  • We considered the general six-dimensional N = (1, 0) supersymmetric gauge theory in the harmonic superspace formulation and studied the dependence of the one-loop divergences on the gauge-fixing parameter

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Summary

Introduction

The study of quantum aspects of the higher-dimensional supersymmetric gauge field theories attracts a wide interest for a long time, mainly because of their use for the low-energy description of diverse sectors of superstring theory (see, e.g., [1, 2]). The present paper generalizes this study to the generic non-abelian N = (1, 0) SYM theory interacting with a set of hypermultiplets in an arbitrary representation of the gauge group. [18,19,20,21,22] was carried out in the framework of the harmonic superfield background field method, which ensures both the classical gauge invariance and N = (1, 0) supersymmetry as manifest symmetries This method was earlier developed for the minimal gauge only. 3 we develop the background superfield method with the gauge-fixing term containing an arbitrary real parameter and derive the formal expression for the corresponding one-loop effective action.

Basic notions
The one-loop effective action
Gauge dependence of the one-loop divergences
Summary

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