{
  "id": "hep-ph/0502225",
  "version": "v2",
  "published": "2005-02-24T12:13:33.000Z",
  "updated": "2005-07-01T07:37:27.000Z",
  "title": "The $s\\bar s$ component of the proton and the strangeness magnetic moment",
  "authors": [
    "B. S. Zou",
    "D. O. Riska"
  ],
  "comment": "4 pages, accepted revised version",
  "journal": "Phys.Rev.Lett. 95 (2005) 072001",
  "doi": "10.1103/PhysRevLett.95.072001",
  "categories": [
    "hep-ph"
  ],
  "abstract": "A complete analysis is given of the implications of the empirical indications for a positive strangeness magnetic moment $\\mu_s$ of the proton on the possible configurations of the $uuds\\bar s$ component of the proton. A positive value for $\\mu_s$ is obtained in the $s\\bar s$ configuration where the $uuds$ subsystem is in an orbitally excited state with $[4]_{[FS]}[22]_F[22]_S$ flavor-spin symmetry, which is likely to have the lowest energy. The configurations in which the $\\bar s$ is orbitally excited, which include the conventional $K^+\\Lambda^0$ configuration, with exception of that in which the $uuds$ component has spin 2, yield negative values for $\\mu_s$. The hidden strangeness analogues of recently proposed quark cluster models for the $\\theta^+$ pentaquark give differing signs for $\\mu_s$.",
  "revisions": [
    {
      "version": "v2",
      "updated": "2005-07-01T07:37:27.000Z"
    }
  ],
  "analyses": {
    "subjects": [
      "12.39.-x",
      "13.40.Em",
      "14.20.Dh"
    ],
    "keywords": [
      "configuration",
      "positive strangeness magnetic moment",
      "hidden strangeness analogues",
      "quark cluster models",
      "complete analysis"
    ],
    "tags": [
      "journal article"
    ],
    "publication": {
      "publisher": "APS",
      "journal": "Phys. Rev. Lett."
    },
    "note": {
      "typesetting": "TeX",
      "pages": 4,
      "language": "en",
      "license": "arXiv",
      "status": "editable",
      "inspire": 677330
    }
  }
}