{
  "annotation_id": "9a70b8cc-3363-4185-ae22-74d0572f661b",
  "date_created": "2026-03-02T18:00:14.165000Z",
  "date_modified": "2026-03-02T18:00:14.165000Z",
  "file_hash": "f6362bdb9324c00eff8d887f22ccafb73fc9fd1d7fc18f2f531e7b2f8b751e1d",
  "private": false,
  "record": {
    "abstract": "We estimate freezeout conditions for $s$, $c$, and $b$ quarks in high energy\nnuclear collisions. Freezeout is due either to loss of thermal contact, or to\nparticles ``wandering\u0027\u0027 out of the region of hot matter. We then develop a\nthermal recombination model in which both single-particle (quark and antiquark)\nand two-particle (quark-antiquark) densities are conserved. Conservation of\ntwo-particle densities is necessary because quarks and antiquarks are always\nproduced in coincidence, so that the local two-particle density can be much\nlarger than the product of the single-particle densities. We use the freezeout\nconditions and recombination model to discuss heavy resonance production at\nzero baryon density in high energy nuclear collisions.",
    "arxiv_id": "nucl-th/9407014",
    "authors": [
      "David Seibert",
      "George Fai"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "doi": "10.1103/PhysRevC.50.2532",
    "journal_ref": "Phys.Rev.C50:2532-2539,1994",
    "title": "Heavy resonance production in high energy nuclear collisions",
    "url": "https://arxiv.org/abs/nucl-th/9407014"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "7b5ce0c6-059a-41f6-841d-2ebcafcf68e1",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}