{
  "annotation_id": "a87fd679-b96e-4cd5-9934-53ebbe4d81ea",
  "date_created": "2026-03-02T18:00:18.509000Z",
  "date_modified": "2026-03-02T18:00:18.509000Z",
  "file_hash": "c145e52d14777e2e3f825525c724ba1d3c3fbcced302da23cce4e9869bb6eb59",
  "private": false,
  "record": {
    "abstract": "The shell model within the $2s1d0g_{7/2}0h_{11/2}$ shell is applied to\ncalculate nuclear structure properties of the even Z=52 - 62, N=82 isotones.\nThe results are compared with experimental data and with the results of a\nquasiparticle random-phase approximation (QRPA) calculation. The interaction\nused in these calculations is a realistic two-body G-matrix interaction derived\nfrom modern meson-exchange potential models for the nucleon-nucleon\ninteraction. For the shell model all the two-body matrix elements are\nrenormalized by the $\\hat{Q}$-box method whereas for the QRPA the effective\ninteraction is defined by the G-matrix.",
    "arxiv_id": "nucl-th/9612064",
    "authors": [
      "A. Holt",
      "T. Engeland",
      "E. Osnes",
      "M. Hjorth-Jensen",
      "J. Suhonen"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/S0375-9474(97)00123-1",
    "journal_ref": "Nucl.Phys. A618 (1997) 107-125",
    "title": "Extended shell-model calculation for even N=82 isotones with realistic   effective interactions",
    "url": "https://arxiv.org/abs/nucl-th/9612064"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "3e09e3b5-13fe-4f93-91d1-283e6f1785a5",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}