{ "id": "1403.0664", "version": "v2", "published": "2014-03-04T02:42:05.000Z", "updated": "2014-03-10T03:33:06.000Z", "title": "Chiral symmetry in $SU(N_c)$ gauge theories at high density", "authors": [ "E. T. Tomboulis" ], "comment": "18 pages, 4 figures, some comments and additional discussion and references included. arXiv admin note: substantial text overlap with arXiv:1304.4678", "categories": [ "hep-th", "hep-lat", "hep-ph" ], "abstract": "We study $SU(N_c)$ lattice gauge theories with $N_f$ flavors of massless staggered fermions in the presence of quark chemical potential $\\mu$. A recent exact result that in the strong coupling limit (vanishing inverse gauge coupling $\\beta$) and for sufficiently large $\\mu$ the theory is in a chiral symmetric phase is here extended into the finite gauge coupling region. A cluster expansion combining a fermion spacelike hopping expansion and a strong coupling plaquette expansion is shown to converge for sufficiently large $\\mu$ and small $\\beta$ at any temperature $T$. All expectations of chirally non-invariant local fermion operators vanish identically, or, equivalently, their correlations cluster exponentially within the expansion implying absence of spontaneous chiral symmetry breaking. The resulting phase at low $T$ may be described as a \"quarkyonic\" matter phase. Some implications for the phase diagram of $SU(N_c)$ theories are discussed.", "revisions": [ { "version": "v2", "updated": "2014-03-10T03:33:06.000Z" } ], "analyses": { "subjects": [ "11.15.Ha", "11.15.Me", "11.30.Rd", "11.10.Mx" ], "keywords": [ "gauge theories", "chiral symmetry", "high density", "local fermion operators vanish" ], "tags": [ "journal article" ], "publication": { "doi": "10.1142/S0217751X14450043", "journal": "International Journal of Modern Physics A", "year": 2014, "month": "Oct", "volume": 29, "number": 25, "pages": 1445004 }, "note": { "typesetting": "TeX", "pages": 18, "language": "en", "license": "arXiv", "status": "editable", "inspire": 1283615, "adsabs": "2014IJMPA..2945004T" } } }