1995/07/31 by Chengxing Zhai, Boris Kastening · 13 citations
Chemistry · Mathematics · Physics and Astronomy · #Black Holes and Theoretical Physics #Chemistry #Combinatorics #Crystallography #Energy (signal processing) #Fermion #Mathematical physics #Mathematics #Particle physics theoretical and experimental studies #Perturbation theory (quantum mechanics) #Physics #Quantum Chromodynamics and Particle Interactions #Quantum mechanics #hep-ph
paper · pdf · doi:10.1103/physrevd.52.7232
published as Phys.Rev. D52 (1995) 7232-7246 · 31 pages, 6 figures, LaTeX; minor beautifications, reference list extended, version to be published in Phys.Rev.D
arxiv created 1995/11/09 · openalex publication_date 1995/12/15 · arxiv updated 2009/11/30 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
We compute the free energy density F for gauge theories, with fermions, at high temperature and zero chemical potential. In the expansion F=T4[c0+c2g2+c3g3+(c4^\ensuremath'lng+c4)g4+(c 5^\ensuremath'g+c5)g5+O(g6)] we determine c5^\ensuremath' and c5 analytically by calculating two- and three-loop diagrams. The g5 term constitutes the first correction to the g3 term and is for the non-Abelian case the last power of g than can be computed within perturbation theory. We find that the g5 term receives no contributions from overlapping double-frequency sums and that c5^\ensuremath' vanishes. \textcopyright 1995 The American Physical Society.