{
  "annotation_id": "4fcfbe0a-ce36-4193-87e9-146c6301dbb5",
  "date_created": "2026-03-02T18:00:10.819000Z",
  "date_modified": "2026-03-02T18:00:10.819000Z",
  "file_hash": "54490c845429721068ed5e92707549047f419f187b0ec43b6a7a1427736c57b9",
  "private": false,
  "record": {
    "abstract": "We study the phase transition from nuclear matter to quark matter within the\nSU(3) quark mean field model and NJL model. The SU(3) quark mean field model is\nused to give the equation of state for nuclear matter, while the equation of\nstate for color superconducting quark matter is calculated within the NJL\nmodel. It is found that at low temperature, the phase transition from nuclear\nto color superconducting quark matter will take place when the density is of\norder 2.5$\\rho_0$ - 5$\\rho_0$. At zero density, the quark phase will appear\nwhen the temperature is larger than about 148 MeV. The phase transition from\nnuclear matter to quark matter is always first order, whereas the transition\nbetween color superconducting quark matter and normal quark matter is second\norder.",
    "arxiv_id": "nucl-th/0610084",
    "authors": [
      "P. Wang",
      "A. W. Thomas",
      "A. G. Williams"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.75.045202",
    "journal_ref": "Phys.Rev.C75:045202,2007",
    "title": "Phase transition from hadronic matter to quark matter",
    "url": "https://arxiv.org/abs/nucl-th/0610084"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "0619e042-40ca-430a-8c1d-5c03a3aee215",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}