{
  "id": "nucl-th/9507013",
  "version": "v1",
  "published": "1995-07-10T03:37:26.000Z",
  "updated": "1995-07-10T03:37:26.000Z",
  "title": "Incompressibility of nuclear matter, and Coulomb and volume-symmetry coefficients of nucleus incompressibility in the relativistic mean field theory",
  "authors": [
    "H. Kouno",
    "T. Mitsumori",
    "N. Noda",
    "K. Koide",
    "A. Hasegawa",
    "M. Nakano"
  ],
  "comment": "PACS numbers: 21.65.+f, 21.30.+y",
  "journal": "Phys.Rev.C53:2542-2545,1996",
  "doi": "10.1103/PhysRevC.53.2542",
  "categories": [
    "nucl-th"
  ],
  "abstract": "The volume coefficient $K$(=incompressibility of the nuclear matter), the Coulomb coefficient $K_c$, and the volume-symmetry coefficient $K_{vs}$ of the nucleus incompressibility are studied in the framework of the relativistic mean field theory, with aid of the scaling model. It is found that $K= 300\\pm 50$MeV is necessary to account for the empirical values of $K_v$, $K_c$, and $K_{vs}$, simultaneously. The result is independent on the detail descriptions of the potential of the $\\sigma$-meson self-interaction and is almost independent of the strength of the $\\omega$-meson self-interaction.",
  "revisions": [
    {
      "version": "v1",
      "updated": "1995-07-10T03:37:26.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "relativistic mean field theory",
      "volume-symmetry coefficient",
      "nucleus incompressibility",
      "nuclear matter",
      "meson self-interaction"
    ],
    "tags": [
      "journal article"
    ],
    "publication": {
      "publisher": "APS",
      "journal": "Phys. Rev. C"
    },
    "note": {
      "typesetting": "TeX",
      "pages": 0,
      "language": "en",
      "license": "arXiv",
      "status": "editable",
      "inspire": 397081
    }
  }
}