{
  "annotation_id": "2e851bd1-dd22-43fd-8c69-70e110aeae6a",
  "date_created": "2026-03-02T18:00:25.663000Z",
  "date_modified": "2026-03-02T18:00:25.663000Z",
  "file_hash": "f9d5a8c57c053569e17a851cd5ed859b74d1caa17fa77362b3462b83c51e2092",
  "private": false,
  "record": {
    "abstract": "We extend a recent billiard model of the nuclear N-body Hamiltonian to\nconsider a finite two-body interaction. This permits a treatment of the\nHamiltonian by a mean field theory, and also allows the possibility to model\nreactions between nuclei. The density and the mean field potential can be\naccurately described by a scaling function which shows the qualitative features\nof the liquid drop picture of the nucleus.",
    "arxiv_id": "nucl-th/9906054",
    "authors": [
      "George F. Bertsch",
      "Thomas Papenbrock",
      "Sanjay Reddy"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/S0375-9474(99)00433-9",
    "journal_ref": "Nucl.Phys. A665 (2000) 285-290",
    "title": "A classical two-body Hamiltonian model and its mean field approximation",
    "url": "https://arxiv.org/abs/nucl-th/9906054"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "7e245771-1090-4d5f-ad78-ce5f9584324d",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}