{ "id": "1307.2803", "version": "v1", "published": "2013-07-10T14:34:11.000Z", "updated": "2013-07-10T14:34:11.000Z", "title": "Potts Models with Invisible States on General Bethe Lattices", "authors": [ "N. Ananikian", "N. Sh. Izmailyan", "D. A. Johnston", "R. Kenna", "R. P. K. C. M. Ranasinghe" ], "journal": "J. Phys. A: Math. Theor. 46 (2013) 385002", "doi": "10.1088/1751-8113/46/38/385002", "categories": [ "cond-mat.stat-mech" ], "abstract": "The number of so-called invisible states which need to be added to the q-state Potts model to transmute its phase transition from continuous to first order has attracted recent attention. In the q=2 case, a Bragg-Williams, mean-field approach necessitates four such invisible states while a 3-regular, random-graph formalism requires seventeen. In both of these cases, the changeover from second- to first-order behaviour induced by the invisible states is identified through the tricritical point of an equivalent Blume-Emery-Griffiths model. Here we investigate the generalised Potts model on a Bethe lattice with z neighbours. We show that, in the q=2 case, r_c(z)=[4 z / 3(z-1)] [(z-1)/(z-2)]^z invisible states are required to manifest the equivalent Blume-Emery-Griffiths tricriticality. When z=3, the 3-regular, random-graph result is recovered, while the infinite z limit delivers the Bragg-Williams, mean-field result.", "revisions": [ { "version": "v1", "updated": "2013-07-10T14:34:11.000Z" } ], "analyses": { "keywords": [ "invisible states", "general bethe lattices", "equivalent blume-emery-griffiths tricriticality", "q-state potts model", "mean-field approach necessitates" ], "tags": [ "journal article" ], "publication": { "journal": "Journal of Physics A Mathematical General", "year": 2013, "month": "Aug", "volume": 46, "number": 31, "pages": 315002 }, "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2013JPhA...46.5002A" } } }