{
  "annotation_id": "a5882a70-a1a1-45be-9c15-b15a4fa37ebd",
  "date_created": "2026-03-02T18:00:14.818000Z",
  "date_modified": "2026-03-02T18:00:14.818000Z",
  "file_hash": "79d10220c6e547cf0e1328ae1f29a6b510ad48a8cdb32f09e6534ebf80043cd0",
  "private": false,
  "record": {
    "abstract": "The role of QCD scales and chiral symmetry in finite nuclei is examined. The\nDirac-Hartree mean-field coupling constants of Nikolaus, Hoch, and Madland\n(NHM) are scaled in accordance with the QCD-based prescription of Manohar and\nGeorgi. Whereas the nine empirically-based coupling constants of NHM span\nthirteen orders of magnitude, the scaled coupling constants are almost all {\\it\nnatural}, being dimensionless numbers of order one. We speculate that this\nresult provides good evidence that QCD and chiral symmetry apply to finite\nnuclei.",
    "arxiv_id": "nucl-th/9512011",
    "authors": [
      "J. L. Friar",
      "D. G. Madland",
      "B. W. Lynn"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "doi": "10.1103/PhysRevC.53.3085",
    "journal_ref": "Phys.Rev.C53:3085-3087,1996",
    "title": "QCD Scales in Finite Nuclei",
    "url": "https://arxiv.org/abs/nucl-th/9512011"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "f21d6b08-6a16-4420-b9cb-9f0f6cf54899",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}