{ "id": "hep-th/0502149", "version": "v2", "published": "2005-02-17T19:10:04.000Z", "updated": "2006-08-14T15:39:24.000Z", "title": "A first order deconfinement transition in large N Yang-Mills theory on a small 3-sphere", "authors": [ "Ofer Aharony", "Joseph Marsano", "Shiraz Minwalla", "Kyriakos Papadodimas", "Mark Van Raamsdonk" ], "comment": "63 pages (40 pages + 2 appendices), 6 figures, harvmac. v2: minor corrections", "journal": "Phys.Rev.D71:125018,2005", "doi": "10.1103/PhysRevD.71.125018", "categories": [ "hep-th", "hep-lat", "hep-ph" ], "abstract": "We give an analytic demonstration that the 3+1 dimensional large N SU(N) pure Yang-Mills theory, compactified on a small 3-sphere so that the coupling constant at the compactification scale is very small, has a first order deconfinement transition as a function of temperature. We do this by explicitly computing the relevant terms in the canonical partition function up to 3-loop order; this is necessary because the leading (1-loop) result for the phase transition is precisely on the borderline between a first order and a second order transition. Since numerical work strongly suggests that the infinite volume large N theory also has a first order deconfinement transition, we conjecture that the phase structure is independent of the size of the 3-sphere. To deal with divergences in our calculations, we are led to introduce a novel method of regularization useful for nonabelian gauge theory on a 3-sphere.", "revisions": [ { "version": "v2", "updated": "2006-08-14T15:39:24.000Z" } ], "analyses": { "subjects": [ "11.15.Pg", "11.10.Wx", "12.38.Mh" ], "keywords": [ "first order deconfinement transition", "nonabelian gauge theory", "pure yang-mills theory", "infinite volume large", "second order transition" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. D" }, "note": { "typesetting": "TeX", "pages": 63, "language": "en", "license": "arXiv", "status": "editable", "inspire": 676951 } } }