{ "id": "hep-ph/9807362", "version": "v2", "published": "1998-07-13T18:26:48.000Z", "updated": "1998-07-16T15:29:55.000Z", "title": "QCD at high Baryon Density and Temperature: Competing Condensates and the Tricritical Point", "authors": [ "J. Berges" ], "comment": "Talk given at the Workshop on QCD at Finite Baryon Density: A Complex System with a Complex Action, Bielefeld, Germany, 27-30 Apr 1998; 7 pages; references added", "journal": "Nucl.Phys.A642:51-57,1998", "doi": "10.1016/S0375-9474(98)00498-9", "categories": [ "hep-ph" ], "abstract": "The phase diagram of strongly interacting matter is explored as a function of temperature and baryon number density. We investigate the possible simultaneous formation of condensates in the conventional quark--anti-quark channel (breaking chiral symmetry) and in a quark--quark channel leading to color superconductivity: the spontaneous breaking of color symmetry via the formation of quark Cooper pairs. We point out that for two massless quark flavors a tricritical point in the phase diagram separates a chiral symmetry restoring first order transition at high densities from the second order transition at high temperatures. Away from the chiral limit this tricritical point becomes a second order phase transition with Ising model exponents, suggesting that a long correlation length may develop in heavy ion collisions in which the phase transition is traversed at the appropriate density.", "revisions": [ { "version": "v2", "updated": "1998-07-16T15:29:55.000Z" } ], "analyses": { "keywords": [ "high baryon density", "tricritical point", "symmetry restoring first order", "competing condensates", "restoring first order transition" ], "tags": [ "journal article" ], "publication": { "publisher": "Elsevier", "journal": "Nucl. Phys. A" }, "note": { "typesetting": "TeX", "pages": 7, "language": "en", "license": "arXiv", "status": "editable", "inspire": 473270 } } }