{
  "annotation_id": "918a8599-d6c8-484c-8b42-bba99e46fd90",
  "date_created": "2026-03-02T18:00:18.831000Z",
  "date_modified": "2026-03-02T18:00:18.831000Z",
  "file_hash": "97fbfbe835689ad10f82a113628c9daa3b9d011ac9d4cc8496891323afa5f45a",
  "private": false,
  "record": {
    "abstract": "We use a large-scale 6 hbar Omega calculation for Li6 with microscopically\nderived two-body interaction to construct the 0 hbar Omega 0p-shell effective\nhamiltonian, electric quadrupole, and magnetic dipole operators. While the E2\nand M1 6 hbar Omega operators are one-body operators with free nucleon charges,\nthe effective operators are two-body operators with substantially different\nrenormalization for the isoscalar and isovector matrix elements, especially for\nthe E2 operator. We show that these operators can be very well approximated by\none-body operators provided that effective proton and neutron charges are used.\nThe obtained effective charges are compatible with those used in\nphenomenological shell-model studies. The two-body part of the effective\noperators is estimated.",
    "arxiv_id": "nucl-th/9612015",
    "authors": [
      "P. Navratil",
      "M. Thoresen",
      "B. R. Barrett"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.55.573",
    "journal_ref": "Phys.Rev.C55:573-576,1997",
    "title": "Microscopic origins of effective charges in the shell model",
    "url": "https://arxiv.org/abs/nucl-th/9612015"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "a02f305a-10a8-4675-a8d0-448cbd0b70b7",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}