{
  "annotation_id": "579dd811-7c48-4a11-9462-d016441e5c2e",
  "date_created": "2026-03-02T18:00:14.164000Z",
  "date_modified": "2026-03-02T18:00:14.164000Z",
  "file_hash": "779f4942c4299974be4bd8d5e7b985597eeca412f1f699abfb9f90699780ac3b",
  "private": false,
  "record": {
    "abstract": "A classical Lagrangian model of the Pauli potential is introduced. It is\nshown that the kinematic kinetic energy ($\\sum \\frac{1}{2} m v^2$) in the model\napproximately reproduces the energy of a free Fermi gas at low temperatures and\nat densities relevant in nuclear collisions with moderate beam energies.\nDifferences between canonical and kinematic quantities are pointed out. The\nPauli potential can be used in transport simulations.",
    "arxiv_id": "nucl-th/9404025",
    "authors": [
      "John J. Neumann",
      "George Fai"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/0370-2693(94)91084-7",
    "journal_ref": "Phys.Lett. B329 (1994) 419-423",
    "title": "Classical Lagrangian Model of the Pauli Principle",
    "url": "https://arxiv.org/abs/nucl-th/9404025"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "b29192c4-6a69-4141-81f3-1f4c0598f9c0",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}