{
  "annotation_id": "e120393b-4d4d-4bfa-8bdf-ad76c03df058",
  "date_created": "2026-03-02T18:00:15.250000Z",
  "date_modified": "2026-03-02T18:00:15.250000Z",
  "file_hash": "9a5d3b31c580da17981af662b8002f275d921b39431ca8d727a068d2a87d5c6a",
  "private": false,
  "record": {
    "abstract": "The relation among the volume coefficient $K$(=incompressibility of the\nnuclear matter), the Coulomb coefficient $K_c$, and the volume-symmetry\ncoefficient $K_{vs}$ of the nucleus incompressibility are studied in the\nframework of the relativistic mean field theory with the excluded volume\neffects of the nucleons, under the assumption of the scaling model. It is found\nthat $K= 300\\pm 50$MeV is necessary to account for the empirical values of $K$,\n$K_c$, and $K_{vs}$, simultaneously, as is in the case of the point-like\nnucleons. The result is independent on the detail descriptions of the potential\nof the $\\sigma$-meson self-interaction and is almost independent on the\nexcluded volume of the nucleons.",
    "arxiv_id": "nucl-th/9507046",
    "authors": [
      "H. Kouno",
      "T. Mitsumori",
      "K. Koide",
      "N. Noda",
      "A. Hasegawa",
      "M. Nakano"
    ],
    "categories": [
      "nucl-th"
    ],
    "title": "Volume, Coulomb, and volume-symmetry coefficients of nucleus   incompressibility in the relativistic mean field theory with the excluded   volume effects",
    "url": "https://arxiv.org/abs/nucl-th/9507046"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "b33790aa-594a-46cd-ab4c-76f590dc3ae0",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}