{ "id": "1206.2312", "version": "v2", "published": "2012-06-11T18:55:08.000Z", "updated": "2012-07-22T09:17:13.000Z", "title": "Logarithmic observables in critical percolation", "authors": [ "Romain Vasseur", "Jesper Lykke Jacobsen", "Hubert Saleur" ], "comment": "11 pages, 2 figures. V2: as published", "journal": "J. Stat. Mech. L07001 (2012)", "doi": "10.1088/1742-5468/2012/07/L07001", "categories": [ "cond-mat.stat-mech", "math-ph", "math.MP" ], "abstract": "Although it has long been known that the proper quantum field theory description of critical percolation involves a logarithmic conformal field theory (LCFT), no direct consequence of this has been observed so far. Representing critical bond percolation as the Q = 1 limit of the Q-state Potts model, and analyzing the underlying S_Q symmetry of the Potts spins, we identify a class of simple observables whose two-point functions scale logarithmically for Q = 1. The logarithm originates from the mixing of the energy operator with a logarithmic partner that we identify as the field that creates two propagating clusters. In d=2 dimensions this agrees with general LCFT results, and in particular the universal prefactor of the logarithm can be computed exactly. We confirm its numerical value by extensive Monte-Carlo simulations.", "revisions": [ { "version": "v2", "updated": "2012-07-22T09:17:13.000Z" } ], "analyses": { "subjects": [ "05.50.+q", "64.60.F-", "64.60.De", "11.25.Hf" ], "keywords": [ "critical percolation", "logarithmic observables", "proper quantum field theory description", "logarithmic conformal field theory", "general lcft results" ], "tags": [ "journal article" ], "publication": { "journal": "Journal of Statistical Mechanics: Theory and Experiment", "year": 2012, "month": "Jul", "volume": 2012, "number": 7 }, "note": { "typesetting": "TeX", "pages": 11, "language": "en", "license": "arXiv", "status": "editable", "inspire": 1118090, "adsabs": "2012JSMTE..07..000V" } } }