{
  "annotation_id": "ce97d6b5-4990-4dd2-a0c0-79bf05ae0aad",
  "date_created": "2026-03-02T18:00:04.912000Z",
  "date_modified": "2026-03-02T18:00:04.912000Z",
  "file_hash": "e365004c236cbdd5152bfedb2458646b93fbb0091f5027f72b1a944507b36dbb",
  "private": false,
  "record": {
    "abstract": "The no-core shell model and the effective interaction $V_{{\\rm low} k}$ can\nboth be derived using the Lee-Suzuki projection operator formalism. The main\ndifference between the two is the choice of basis states that define the model\nspace. The effective interaction $V_{{\\rm low} k}$ can also be derived using\nthe renormalization group. That renormalization group derivation can be\nextended in a straight forward manner to also include the no-core shell model.\nIn the nuclear matter limit the no-core shell model effective interaction in\nthe two-body approximation reduces identically to $V_{{\\rm low} k}$. The same\nconsiderations apply to the Bloch-Horowitz version of the shell model and the\nrenormalization group treatment of two-body scattering by Birse, McGovern and\nRichardson.",
    "arxiv_id": "nucl-th/0504070",
    "authors": [
      "B. K. Jennings"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1209/epl/i2005-10222-0",
    "journal_ref": "Europhys.Lett. 72 (2005) 216-220",
    "title": "The Shell Model, the Renormalization Group and the Two-Body Interaction",
    "url": "https://arxiv.org/abs/nucl-th/0504070"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "ff40f8d9-78b5-4676-8481-c1026249c163",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}