{
  "annotation_id": "44092c53-296e-479c-8633-7aec4437e5a7",
  "date_created": "2026-03-02T18:00:21.657000Z",
  "date_modified": "2026-03-02T18:00:21.657000Z",
  "file_hash": "afbb7068118acb0efaed960222d10ee25e2b021c78c3cbd95a46d8e791fa3bcb",
  "private": false,
  "record": {
    "abstract": "Shell corrections of finite, spherical, one-body potentials are analyzed\nusing a smoothing procedure which properly accounts for the contribution from\nthe particle continuum, i.e., unbound states. Since the plateau condition for\nthe smoothed single-particle energy seldom holds, a new recipe is suggested for\nthe definition of the shell correction. The generalized Strutinsky smoothing\nprocedure is compared with the results of the semi-classical Wigner-Kirkwood\nexpansion. A good agreement has been found for weakly bound nuclei in the\nvicinity of the proton drip line. However, some deviations remain for extremely\nneutron-rich systems due to the pathological behavior of the semi-classical\nlevel density around the particle threshold.",
    "arxiv_id": "nucl-th/9802014",
    "authors": [
      "T. Vertse",
      "A. T. Kruppa",
      "R. J. Liotta",
      "W. Nazarewicz",
      "N. Sandulescu",
      "T. R. Werner"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.57.3089",
    "journal_ref": "Phys.Rev.C57:3089-3098,1998",
    "title": "Shell corrections for finite depth potentials: Particle continuum   effects",
    "url": "https://arxiv.org/abs/nucl-th/9802014"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "4fa9ccb3-9ba7-4c15-b5f8-cbf96fbea8ff",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}