{
  "id": "cond-mat/0107225",
  "version": "v3",
  "published": "2001-07-11T10:52:48.000Z",
  "updated": "2001-07-25T09:06:24.000Z",
  "title": "On the Finite Size Scaling in Disordered Systems",
  "authors": [
    "H. Chamati",
    "E. Korutcheva",
    "N. S. Tonchev"
  ],
  "comment": "21 pages, 2 figures, submitted to the Physcal Review E",
  "doi": "10.1103/PhysRevE.65.026129",
  "categories": [
    "cond-mat.stat-mech"
  ],
  "abstract": "The critical behavior of a quenched random hypercubic sample of linear size $L$ is considered, within the ``random-$T_{c}$'' field-theoretical mode, by using the renormalization group method. A finite-size scaling behavior is established and analyzed near the upper critical dimension $d=4-\\epsilon$ and some universal results are obtained. The problem of self-averaging is clarified for different critical regimes.",
  "revisions": [
    {
      "version": "v3",
      "updated": "2001-07-25T09:06:24.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "finite size scaling",
      "disordered systems",
      "quenched random hypercubic sample",
      "renormalization group method",
      "upper critical dimension"
    ],
    "tags": [
      "journal article"
    ],
    "publication": {
      "publisher": "APS",
      "journal": "Phys. Rev. E"
    },
    "note": {
      "typesetting": "TeX",
      "pages": 21,
      "language": "en",
      "license": "arXiv",
      "status": "editable"
    }
  }
}