{
  "id": "cond-mat/0207300",
  "version": "v1",
  "published": "2002-07-11T16:30:46.000Z",
  "updated": "2002-07-11T16:30:46.000Z",
  "title": "Why temperature chaos in spin glasses is hard to observe",
  "authors": [
    "T. Aspelmeier",
    "A. J. Bray",
    "M. A. Moore"
  ],
  "comment": "4 pages, 6 figures",
  "journal": "Phys. Rev. Lett. 89, 197202 (2002)",
  "doi": "10.1103/PhysRevLett.89.197202",
  "categories": [
    "cond-mat.dis-nn",
    "cond-mat.stat-mech"
  ],
  "abstract": "The overlap length of a three-dimensional Ising spin glass on a cubic lattice with Gaussian interactions has been estimated numerically by transfer matrix methods and within a Migdal-Kadanoff renormalization group scheme. We find that the overlap length is large, explaining why it has been difficult to observe spin glass chaos in numerical simulations and experiment.",
  "revisions": [
    {
      "version": "v1",
      "updated": "2002-07-11T16:30:46.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "spin glasses",
      "temperature chaos",
      "overlap length",
      "migdal-kadanoff renormalization group scheme",
      "transfer matrix methods"
    ],
    "tags": [
      "journal article"
    ],
    "publication": {
      "publisher": "APS",
      "journal": "Phys. Rev. Lett."
    },
    "note": {
      "typesetting": "TeX",
      "pages": 4,
      "language": "en",
      "license": "arXiv",
      "status": "editable"
    }
  }
}