{ "id": "1412.2448", "version": "v1", "published": "2014-12-08T05:02:23.000Z", "updated": "2014-12-08T05:02:23.000Z", "title": "Critical Point Scaling of Ising Spin Glasses in a Magnetic Field", "authors": [ "Joonhyun Yeo", "M. A. Moore" ], "comment": "9 pages, 12 figures", "categories": [ "cond-mat.dis-nn", "cond-mat.stat-mech" ], "abstract": "Critical point scaling in a field $H$ applies for the limits $t\\to 0$, (where $t=T/T_c-1$) and $H\\to 0$ but with the ratio $R=t/H^{2/\\Delta}$ finite. $\\Delta$ is a critical exponent of the zero-field transition. We study the replicon correlation length $\\xi$ and from it the crossover scaling function $f(R)$ defined via $1/(\\xi H^{4/(d+2-\\eta)}) \\sim f(R)$. We have calculated analytically $f(R)$ for the mean-field limit of the Sherrington-Kirkpatrick model. In dimension d=3 we have determined the exponents and the critical scaling function $f(R)$ within two versions of the Migdal-Kadanoff (MK) renormalization group procedure. One of the MK versions gives results for $f(R)$ in d=3 in reasonable agreement with those of the Monte Carlo simulations at the values of R for which they can be compared. If there were a de Almeida-Thouless (AT) line for $d \\le 6$ it would appear as a zero of the function $f(R)$ at some negative value of R, but there is no evidence for such behavior. This is consistent with the arguments that there should be no AT line for $d \\le 6$, which we review.", "revisions": [ { "version": "v1", "updated": "2014-12-08T05:02:23.000Z" } ], "analyses": { "subjects": [ "75.10.Nr", "75.40.Cx", "05.50.+q", "75.50.Lk" ], "keywords": [ "critical point scaling", "ising spin glasses", "magnetic field", "monte carlo simulations", "renormalization group procedure" ], "publication": { "doi": "10.1103/PhysRevB.91.104432", "journal": "Physical Review B", "year": 2015, "month": "Mar", "volume": 91, "number": 10, "pages": 104432 }, "note": { "typesetting": "TeX", "pages": 9, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2015PhRvB..91j4432Y" } } }