{ "id": "1409.1374", "version": "v1", "published": "2014-09-04T09:15:41.000Z", "updated": "2014-09-04T09:15:41.000Z", "title": "Revisiting the nonperturbative renormalization-group approach to the Kosterlitz-Thouless transition", "authors": [ "P. Jakubczyk", "N. Dupuis", "B. Delamotte" ], "comment": "10 pages, 10 figures", "categories": [ "cond-mat.stat-mech" ], "abstract": "We revisit the two-dimensional linear O(2) model ($\\varphi^4$ theory) in the framework of the nonperturbative renormalization-group. From the flow equations obtained in the derivative expansion to second order and with optimization of the infrared regulator, we find a transition between a high-temperature (disordered) phase and a low-temperature phase displaying a line of fixed points and algebraic order. We obtain a picture in agreement with the standard theory of the Kosterlitz-Thouless (KT) transition and reproduce the universal features of the transition. In particular, we find the anomalous dimension $\\eta(\\Tkt)\\simeq 0.24$ and the stiffness jump $\\rho_s(\\Tkt^-)\\simeq 0.64$ at the transition temperature $\\Tkt$, in very good agreement with the exact results $\\eta(\\Tkt)=1/4$ and $\\rho_s(\\Tkt^-)=2/\\pi$, as well as an essential singularity of the correlation length in the high-temperature phase as $T\\to \\Tkt$.", "revisions": [ { "version": "v1", "updated": "2014-09-04T09:15:41.000Z" } ], "analyses": { "subjects": [ "05.70.Fh", "05.10.Cc", "74.20.-z" ], "keywords": [ "nonperturbative renormalization-group approach", "kosterlitz-thouless transition", "two-dimensional linear", "essential singularity", "exact results" ], "tags": [ "journal article" ], "publication": { "doi": "10.1103/PhysRevE.90.062105", "journal": "Physical Review E", "year": 2014, "month": "Dec", "volume": 90, "number": 6, "pages": "062105" }, "note": { "typesetting": "TeX", "pages": 10, "language": "en", "license": "arXiv", "status": "editable", "inspire": 1315972, "adsabs": "2014PhRvE..90f2105J" } } }