{
  "annotation_id": "2b04d61e-f47e-46b1-8c83-efb9a7b52258",
  "date_created": "2026-03-02T18:00:01.195000Z",
  "date_modified": "2026-03-02T18:00:01.195000Z",
  "file_hash": "68074afc5df5db96b1c03f10c3a9e870c9d606873de2c07179db4bed330830d2",
  "private": false,
  "record": {
    "abstract": "We use a chiral SU(3) quark mean field model to study the properties of\nnuclear systems at finite temperature. The liquid-gas phase transition of\nsymmetric and asymmetric nuclear matter is discussed. For two formulations of\nthe model the critical temperature, $T_c$, for symmetric nuclear matter is\nfound to be 15.8 MeV and 17.9 MeV. These values are consistent with those\nderived from recent experiments. The limiting temperatures for finite nuclei\nare in good agreement with the experimental points.",
    "arxiv_id": "nucl-th/0407057",
    "authors": [
      "P. Wang",
      "D. B. Leinweber",
      "A. W. Thomas",
      "A. G. Williams"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/j.nuclphysa.2004.10.012",
    "journal_ref": "Nucl.Phys.A748:226-240,2005",
    "title": "Liquid-gas phase transition and Coulomb instability of asymmetric   nuclear systems",
    "url": "https://arxiv.org/abs/nucl-th/0407057"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "0857ab15-3193-4e28-8ba5-429d236bb44c",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}