{
  "id": "cond-mat/0110017",
  "version": "v1",
  "published": "2001-10-01T08:26:08.000Z",
  "updated": "2001-10-01T08:26:08.000Z",
  "title": "Spin-Glass and Chiral-Glass Transitions in a $\\pm J$ Heisenberg Spin-Glass Model in Three Dimensions",
  "authors": [
    "Tota Nakamura",
    "Shin-ichi Endoh"
  ],
  "comment": "4 pages, 2 figures",
  "journal": "J. Phys. Soc. Jpn. 71, 2113 (2002).",
  "doi": "10.1143/JPSJ.71.2113",
  "categories": [
    "cond-mat.dis-nn"
  ],
  "abstract": "The three-dimensional $\\pm J$ Heisenberg spin-glass model is investigated by the non-equilibrium relaxation method from the paramagnetic state. Finite-size effects in the non-equilibrium relaxation are analyzed, and the relaxation functions of the spin-glass susceptibility and the chiral-glass susceptibility in the infinite-size system are obtained. The finite-time scaling analysis gives the spin-glass transition at $T_{\\rm sg}/J=0.21_{-0.02}^{+0.01}$ and the chiral-glass transition at $T_{\\rm cg}/J=0.22_{-0.03}^{+0.01}$. The results suggest that both transitions occur simultaneously. The critical exponent of the spin-glass susceptibility is estimated as $\\gamma_{\\rm sg}= 1.7 \\pm 0.3$, which makes an agreement with the experiments of the insulating and the canonical spin-glass materials.",
  "revisions": [
    {
      "version": "v1",
      "updated": "2001-10-01T08:26:08.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "heisenberg spin-glass model",
      "chiral-glass transition",
      "spin-glass susceptibility",
      "dimensions",
      "non-equilibrium relaxation method"
    ],
    "tags": [
      "journal article"
    ],
    "publication": {
      "journal": "Journal of the Physical Society of Japan",
      "year": 2002,
      "month": "Sep",
      "volume": 71,
      "number": 9,
      "pages": 2113
    },
    "note": {
      "typesetting": "TeX",
      "pages": 4,
      "language": "en",
      "license": "arXiv",
      "status": "editable",
      "adsabs": "2002JPSJ...71.2113N"
    }
  }
}