{
  "annotation_id": "64efa119-7183-4aa8-8cf9-fda9d001a58c",
  "date_created": "2026-03-02T18:00:01.499000Z",
  "date_modified": "2026-03-02T18:00:01.499000Z",
  "file_hash": "c1088b29469aa389e3e9580a81a32b146e1b4d7101d3abd3483bb2df9c5a9138",
  "private": false,
  "record": {
    "abstract": "We discuss a relation between the\n  QCD thermodynamics obtained from a statistical analysis of particle\nproduction in heavy ion collisions at SPS and RHIC energies and recent LGT\nresults at finite chemical potential. We show that basic thermodynamic\nproperties obtained from the phenomenological statistical operator of a hadron\nresonance gas that describes particle yields in heavy ion collisions are\nconsistent with recent LGT results. We argue that for $T\\leq T_c$ the equation\nof state derived from\n  Monte--Carlo simulations of two quark--flavor QCD at finite chemical\npotential can be well described by a hadron resonance gas when using the same\nset of approximations as used in LGT calculations. We examine the influence of\na finite quark mass on the position of the deconfinement transition in\ntemperature and chemical potential plane.",
    "arxiv_id": "nucl-th/0404009",
    "authors": [
      "K. Redlich",
      "F. Karsch",
      "A. Tawfik"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1088/0954-3899/30/8/106",
    "journal_ref": "J.Phys. G30 (2004) S1271-S1274",
    "title": "Heavy ion collisions and lattice QCD at finite baryon density",
    "url": "https://arxiv.org/abs/nucl-th/0404009"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "b4a6f917-52aa-48a2-90f2-00bee615f9c8",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}