{
  "annotation_id": "b6b05c9b-8fc7-4017-bf70-93d369b1427d",
  "date_created": "2026-03-02T18:00:04.336000Z",
  "date_modified": "2026-03-02T18:00:04.336000Z",
  "file_hash": "659c63ca7ac188bd26ed5850fa1eadf0c357d53228465e2dde5ca09a934126c0",
  "private": false,
  "record": {
    "abstract": "Phase diagram of strongly interacting matter is discussed within the exactly\nsolvable statistical model of the quark-gluon bags. The model predicts two\nphases of matter: the hadron gas at a low temperature T and baryonic chemical\npotential muB, and the quark-gluon gas at a high T and/or muB. The nature of\nthe phase transition depends on a form of the bag mass-volume spectrum (its\npre-exponential factor), which is expected to change with the muB/T ratio. It\nis therefore likely that the line of the 1st} order transition at a high muB/T\nratio is followed by the line of the 2nd order phase transition at an\nintermediate muB/T, and then by the lines of \"higher order transitions\" at a\nlow muB/T.",
    "arxiv_id": "nucl-th/0505050",
    "authors": [
      "M. I. Gorenstein",
      "M. Gazdzicki",
      "W. Greiner"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.72.024909",
    "journal_ref": "Phys.Rev.C72:024909,2005",
    "title": "Critical line of the deconfinement phase transition",
    "url": "https://arxiv.org/abs/nucl-th/0505050"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "805a1801-7789-4fe5-b80f-f2cf37b44a5a",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}