{
  "annotation_id": "d18ad192-cacc-41d2-8654-15c8650623cd",
  "date_created": "2026-03-02T18:00:22.101000Z",
  "date_modified": "2026-03-02T18:00:22.101000Z",
  "file_hash": "af23c5b612e32ea2555cf53d8d7b05e85a2c9b08f181b8d0b439a8c1f01571d4",
  "private": false,
  "record": {
    "abstract": "The position of the two-proton drip line has been calculated for even-even\nnuclei with $10 \\leq Z \\leq 82$ in the framework of the relativistic mean-field\n(RMF) theory. The current model uses the NL3 effective interaction in the\nmean-field Lagrangian and describes pairing correlations in the\nBardeen-Cooper-Schrieffer (BCS) formalism. The predictions of the RMF theory\nare compared with those of the Hartree-Fock+BCS approach (with effective force\nSkyrme SIII) and the finite-range droplet model (FRDM) and with the available\nexperimental information.",
    "arxiv_id": "nucl-th/9806019",
    "authors": [
      "G. A. Lalazissis",
      "S. Raman"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.58.1467",
    "journal_ref": "Phys.Rev.C58:1467-1472,1998",
    "title": "Proton drip-line nuclei in relativistic mean-field theory",
    "url": "https://arxiv.org/abs/nucl-th/9806019"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "c786dbc1-4a30-45c8-a8b9-999422e72445",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}