Vacuum energy for Yang-Mills fields in $R^d\times S^1$: One-loop, two-loop, and beyond

TL;DR

This paper calculates the vacuum energy of Yang-Mills fields in higher-dimensional space-times up to two-loop order, introducing an approximation method to efficiently estimate higher-loop contributions relevant for Kaluza-Klein theories and quark-gluon plasma.

Contribution

It develops a novel approximation method to evaluate higher-loop effects in vacuum energy calculations for Yang-Mills fields in higher dimensions.

Findings

Successfully reproduces two-loop contributions in small coupling limit.

Provides an effective approach for higher-loop calculations in complex systems.

Applicable to Kaluza-Klein theories and finite temperature-density systems.

Abstract

The vacuum energy is calculated for Yang-Mills (YM) system defined in $D$ dimensional space-time of $S^1\times R^d$ ($D=d+1$), where the possibility of the YM fields to acquire the vacuum expectation values on $S^1$ is taken into account. The vacuum energy has already been obtained to the order of one-loop in many people. Here we calculate the vacuum energy in $D$ dimensions to two-loop order. With an intention to reach higher loops, an approximation method is proposed, which is especially effective in higher dimensions. By this method, we can treat the higher-loop contributions of YM interactions as easily as we treat one-loop effect. As a check, we show reproduction of the two-loop contribution ($D$-dependence of the coefficient as well as the functional form) when the coupling constant is small. This approximation method is useful not only for the Kaluza-Klein theories but also for the finite temperature-density system (as a quark-gluon plasma).