{ "id": "hep-ph/9409434", "version": "v1", "published": "1994-09-28T19:58:52.000Z", "updated": "1994-09-28T19:58:52.000Z", "title": "Solution to the Perturbative Infrared Catastrophe of Hot Gauge Theories", "authors": [ "Eric Braaten" ], "comment": "11 pages LaTeX, NUHEP-TH-94-24", "journal": "Phys.Rev.Lett.74:2164-2167,1995", "doi": "10.1103/PhysRevLett.74.2164", "categories": [ "hep-ph", "hep-lat", "hep-th" ], "abstract": "The free energy of a nonabelian gauge theory at high temperature $T$ can be calculated to order $g^5$ using resummed perturbation theory, but the method breaks down at order $g^6$. A new method is developed for calculating the free energy to arbitrarily high accuracy in the high temperature limit. It involves the construction of a sequence of two effective field theories by first integrating out the momentum scale $T$ and then integrating out the momentum scale $g T$. The free energy decomposes into the sum of three terms, corresponding to the momentum scales $T$, $gT$, and $g^2T$. The first term can be calculated as a perturbation series in $g^2(T)$, where $g(T)$ is the running coupling constant. The second term in the free energy can be calculated as a perturbation series in $g(T)$, beginning at order $g^3$. The third term can also be expressed as a series in $g(T)$ beginning at order $g^6$, with coefficients that can be calculated using lattice simulations of 3-dimensional QCD. Leading logarithms of $T/(gT)$ and of $gT/(g^2T)$ can be summed up using renormalization group equations.", "revisions": [ { "version": "v1", "updated": "1994-09-28T19:58:52.000Z" } ], "analyses": { "keywords": [ "gauge theory", "hot gauge theories", "perturbative infrared catastrophe", "momentum scale", "perturbation series" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. Lett." }, "note": { "typesetting": "LaTeX", "pages": 11, "language": "en", "license": "arXiv", "status": "editable", "inspire": 377416 } } }