{
  "annotation_id": "3b30b0f2-2c53-4f02-9894-9e96c4ec3027",
  "date_created": "2026-03-02T18:00:18.959000Z",
  "date_modified": "2026-03-02T18:00:18.959000Z",
  "file_hash": "c2cd4427090b6ee91559fc3fc8aee8be9f96fc2510c743d578fd9ac0046bd7bc",
  "private": false,
  "record": {
    "abstract": "The quark-meson coupling (QMC) model, which has been successfully used to\ndescribe the properties of both finite nuclei and infinite nuclear matter, is\napplied to a study of $\\Lambda$ hypernuclei. With the assumption that the\n(self-consistent) exchanged scalar, and vector, mesons couple only to the u and\nd quarks, a very weak spin-orbit force in the $\\Lambda$-nucleus interaction is\nachieved automatically. This is a direct consequence of the SU(6) quark model\nwave function of the $\\Lambda$ used in the QMC model. Possible implications and\nextensions of the present investigation are also discussed.",
    "arxiv_id": "nucl-th/9701047",
    "authors": [
      "K. Tsushima",
      "K. Saito",
      "A. W. Thomas"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "doi": "10.1016/S0370-2693(97)00944-1",
    "journal_ref": "Phys.Lett.B411:9-18,1997; Erratum-ibid.B421:413,1998",
    "title": "Self-consistent description of $\\Lambda$ hypernuclei in the quark-meson   coupling model",
    "url": "https://arxiv.org/abs/nucl-th/9701047"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "73ade4b2-ce50-4ff0-a179-a428b9eb231c",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}