{ "id": "cond-mat/0603137", "version": "v1", "published": "2006-03-06T14:41:58.000Z", "updated": "2006-03-06T14:41:58.000Z", "title": "The fluctuation-dissipation relation in an Ising model without detailed balance", "authors": [ "Natascia Andrenacci", "Federico Corberi", "Eugenio Lippiello" ], "comment": "17 pages, 15 figures. To appear on Physical Review E", "journal": "Phys. Rev. E 73, 046124 (2006)", "doi": "10.1103/PhysRevE.73.046124", "categories": [ "cond-mat.stat-mech" ], "abstract": "We consider the modified Ising model introduced by de Oliveira et al. [J.Phys.A {\\bf 26}, 2317 (1993)], where the temperature depends locally on the spin configuration and detailed balance and local equilibrium are not obeyed. We derive a relation between the linear response function and correlation functions which generalizes the fluctuation-dissipation theorem. In the stationary states of the model, which are the counterparts of the Ising equilibrium states, the fluctuation-dissipation theorem breaks down due to the lack of time reversal invariance. In the non-stationary phase ordering kinetics the parametric plot of the integrated response function $\\chi (t,t_w)$ versus the autocorrelation function is different from that of the kinetic Ising model. However, splitting $\\chi (t,t_w)$ into a stationary and an aging term $\\chi (t,t_w)=\\chi_{st}(t-t_w)+\\chi_{ag}(t,t_w)$, we find $\\chi_{ag}(t,t_w)\\sim t_w^{-a_\\chi}f(t/t_w)$, and a numerical value of $a_\\chi $ consistent with $a_\\chi =1/4$, as in the kinetic Ising model.", "revisions": [ { "version": "v1", "updated": "2006-03-06T14:41:58.000Z" } ], "analyses": { "keywords": [ "detailed balance", "fluctuation-dissipation relation", "kinetic ising model", "linear response function", "fluctuation-dissipation theorem breaks" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. E" }, "note": { "typesetting": "TeX", "pages": 17, "language": "en", "license": "arXiv", "status": "editable" } } }