{
  "annotation_id": "4ac0448b-6dcb-4af7-b220-fdb69701f49d",
  "date_created": "2026-03-02T18:00:14.166000Z",
  "date_modified": "2026-03-02T18:00:14.166000Z",
  "file_hash": "33256707d580280eb71e02e054c8646d3564a329ff982b486f261c06379e0ef3",
  "private": false,
  "record": {
    "abstract": "The phenomenon of collective flow in relativistic heavy ion collisions is\nstudied using the hadronic cascade model ARC. Direct comparison is made to data\ngathered at the Bevalac, for Au+Au at $p=1-2$ GeV/c. In contrast to the\nstandard lore about the cascade model, collective flow is well described\nquantitatively without the need for explicit mean field terms to simulate the\nnuclear equation of state. Pion collective flow is in the opposite direction to\nnucleon flow as is that of anti-nucleons and other produced particles. Pion and\nnucleon flow are predicted at AGS energies also, where, in light of the higher\nbaryon densities achieved, we speculate that equation of state effects may be\nobservable.",
    "arxiv_id": "nucl-th/9405017",
    "authors": [
      "David E. Kahana",
      "Declan Keane",
      "Yang Pang",
      "Tom Schlagel",
      "Shan Wang"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevLett.74.4404",
    "journal_ref": "Phys.Rev.Lett. 74 (1995) 4404-4407",
    "title": "Collective Flow from the Intranuclear Cascade Model",
    "url": "https://arxiv.org/abs/nucl-th/9405017"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "39f3ab80-f4d4-4fac-be23-32f9a0a53661",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}