{
  "annotation_id": "cbc754b4-ecff-4d20-8d51-dc733dbadba1",
  "date_created": "2026-03-02T18:00:15.537000Z",
  "date_modified": "2026-03-02T18:00:15.537000Z",
  "file_hash": "74fbdc9351219cd8cd26f82df4e2bed5f88a466277200dc9f80af5e40aba8658",
  "private": false,
  "record": {
    "abstract": "The volume coefficient $K$(=incompressibility of the nuclear matter), the\nCoulomb coefficient $K_c$, and the volume-symmetry coefficient $K_{vs}$ of the\nnucleus incompressibility are studied in the framework of the relativistic mean\nfield theory, with aid of the scaling model. It is found that $K= 300\\pm 50$MeV\nis necessary to account for the empirical values of $K_v$, $K_c$, and $K_{vs}$,\nsimultaneously. The result is independent on the detail descriptions of the\npotential of the $\\sigma$-meson self-interaction and is almost independent of\nthe strength of the $\\omega$-meson self-interaction.",
    "arxiv_id": "nucl-th/9507013",
    "authors": [
      "H. Kouno",
      "T. Mitsumori",
      "N. Noda",
      "K. Koide",
      "A. Hasegawa",
      "M. Nakano"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.53.2542",
    "journal_ref": "Phys.Rev.C53:2542-2545,1996",
    "title": "Incompressibility of nuclear matter, and Coulomb and volume-symmetry   coefficients of nucleus incompressibility in the relativistic mean field   theory",
    "url": "https://arxiv.org/abs/nucl-th/9507013"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "b7cc2a8f-2470-43ce-a362-05c9fd7e9e72",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}