{
  "annotation_id": "ced26690-bdf6-480d-9bb7-821a22c2cdad",
  "date_created": "2026-03-02T18:00:25.479000Z",
  "date_modified": "2026-03-02T18:00:25.479000Z",
  "file_hash": "4d80f1c50608c218683bbe9796be834136ee0ba02611e070d2c96124fae5bfc7",
  "private": false,
  "record": {
    "abstract": "We formulate a lattice Hamiltonian model for intermediate energy heavy ion\ncollisions. Our approach incorporates a momentum-dependent nuclear mean field\nthat yields an optical potential that agrees with proton-nucleus experiments\nand that also receives support from measurements involving heavy ions. We\nemphasize the precision of our numerical results in connection with energy and\nmomentum conservation. We first outline the static properties of our solutions,\nafter which we consider recent stopping power results for heavy ion collisions.\nThe results obtained with different types of nuclear mean fields are compared\nwith each other. Consequences of the stopping power data on the nuclear\nequation of state are outlined.",
    "arxiv_id": "nucl-th/9901019",
    "authors": [
      "Declan Persram",
      "Charles Gale"
    ],
    "categories": [
      "nucl-th"
    ],
    "title": "Splintering central nuclear collisions with a momentum-dependent lattice   Hamiltonian theory",
    "url": "https://arxiv.org/abs/nucl-th/9901019"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "e9fe0c84-eb34-4846-a2f1-36cf4f225232",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}