{
  "annotation_id": "57d3c7ae-9a86-418a-9440-6d47b686b47b",
  "date_created": "2026-03-02T18:00:22.032000Z",
  "date_modified": "2026-03-02T18:00:22.032000Z",
  "file_hash": "06f7003b3d20b32c518af05d2699eedef11d1635ec08e3dbafaa04991aa06a0b",
  "private": false,
  "record": {
    "abstract": "We try to explain the differences in the 6He dipole strength function in\nrefs. [1] and [2]. We perform the full basis calculation of the strength\nfunction with the same renormalized interaction as in [1] and show that the\nsize of the basis, needed for converged calculations of the 6He continuum\nspectrum, is much larger than that for the discrete spectrum. The renormalized\ninteraction of [1] therefore cannot be used for the continuum spectrum\ncalculations with the same basis as for the ground state.",
    "arxiv_id": "nucl-th/9801033",
    "authors": [
      "D. V. Fedorov",
      "A. Cobis",
      "A. S. Jensen"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.59.554",
    "journal_ref": "Phys.Rev.C59:554-555,1999",
    "title": "Comment on \"New modes of halo excitations in the 6He nucleus\"",
    "url": "https://arxiv.org/abs/nucl-th/9801033"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "5c92b45b-5881-4e2c-be63-d5bb1e0c34fc",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}