{
  "annotation_id": "966c98ef-74fa-406a-bb72-8fa6c1b7df42",
  "date_created": "2026-03-02T18:00:15.305000Z",
  "date_modified": "2026-03-02T18:00:15.305000Z",
  "file_hash": "35678f15bde94106e70a08c764342a3d8bd604337e8388d0e06fdf40a64c29f4",
  "private": false,
  "record": {
    "abstract": "We study halo nuclei using a two-frequency shell-model approach employing\nwave functions of two different oscillator constants $\\hbar\\omega_{in}$ and\n$\\hbar\\omega_{out}$, the former for the inner orbits and the latter for the\nhalo (outer) orbits. An initial application has been made for the halo nuclei\n$^6$He and $^6$Li, with $0s_{1/2}$ taken as the inner and ( $0p_{3/2}$,\n$0p_{1/2}$) as the halo orbits. Starting from the Paris NN interaction, we have\nderived a G-matrix folded-diagram effective interaction for this two-frequency\nmodel space, using an essentially exact treatment for the Pauli exclusion\noperator for the G-matrix. While keeping $\\hbar\\omega_{in}$ fixed, we have\nperformed calculations with different choices for $\\hbar\\omega_{out}$, treating\nit as a variation parameter. For $\\hbar\\omega_{in}=19.7 MeV$ and\n$\\hbar\\omega_{out}=8.2 MeV$, our calculated valence energies for $^6$He and\n$^6$Li are -2.77 and -3.55 Mev, respectively, both in good agreement with\nexperiments. The importance of certain three-body-force diagrams is discussed.",
    "arxiv_id": "nucl-th/9603045",
    "authors": [
      "T. T. S. Kuo",
      "H. M\u00fcther",
      "K. Amir-Azimi-Nili"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/0375-9474(96)00205-9",
    "journal_ref": "Nucl.Phys. A606 (1996) 15-26; Erratum-ibid. A611 (1996) 587",
    "title": "Realistic effective interactions for halo nuclei",
    "url": "https://arxiv.org/abs/nucl-th/9603045"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "1b1e6ea3-6d3c-4e22-ae31-4e13303f666e",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}