The Free Energy of Hot Gauge Theories with Fermions Through g^5

Abstract

We compute the free energy density $F$ for gauge theories, with fermions, at high temperature and zero chemical potential. In the expansion $F=T^4[c_0+c_2{g}^2+c_3{g}^3+(c_4^{\prime }\ln g+c_4)g^4+(c_5^{\prime }\ln g+c_5)g^5+O(g^6)]$, we determine $c_5^{\prime }$ and $c_5$ analytically by calculating two- and three-loop diagrams. The $g^5$ term constitutes the first correction to the $g^3$ term and is for the non-Abelian case the last power of $g$ that can be computed within perturbation theory. We find that the $g^5$ term receives no contributions from overlapping double-frequency sums and that $c_5^{\prime }$ vanishes.

arXiv comment31 pages, 6 figures, LaTeX; minor beautifications, reference list extended, version to be published in Phys.Rev.D

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