{
  "annotation_id": "3784772e-57ed-40f7-8e7f-e474528e666c",
  "date_created": "2026-03-02T18:00:11.330000Z",
  "date_modified": "2026-03-02T18:00:11.330000Z",
  "file_hash": "aec73f10678a488682b6619c20875f50b593fd421a40dbb8f017d32d1475c7de",
  "private": false,
  "record": {
    "abstract": "Two different approximation schemes for the self-consistent solution of the\nrelativistic Brueckner-Hartree-Fock equation for finite nuclei are discussed\nusing realistic One-Boson-Exchange potentials. In a first scheme, the effects\nof correlations are deduced from a study of nuclear matter and parameterized in\nterms of an effective $\\sigma$, $\\omega$ and $\\pi$ exchange. Employing this\neffective interaction relativistic Hartree-Fock equations are solved for finite\nnuclei \\osi , \\caf\\ and \\cafe . In the second approach the effect of\ncorrelations are treated in the Brueckner-Hartree-Fock approximation directly\nfor the finite nuclei, but the modifications of the Dirac spinors in the medium\nare derived from nuclear matter assuming a local-density approximation. Both\napproaches yield rather similar results for binding energies and radii in fair\nagreement with experimental data. The importance of the density dependent\ncorrelation effects is demonstrated and different ingredients to the spin-orbit\nsplitting in the shell-model of the nucleus are discussed.",
    "arxiv_id": "nucl-th/9309029",
    "authors": [
      "R. Fritz",
      "H. M\u00fcther"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.49.633",
    "title": "NN Correlations and Relativistic Hartree Fock in Finite Nuclei",
    "url": "https://arxiv.org/abs/nucl-th/9309029"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "0daa08a4-3efc-488b-a48e-b4796173ca00",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}