{
  "annotation_id": "f3bfbb9b-250a-4506-b681-8edb7c3085de",
  "date_created": "2026-03-02T18:00:18.518000Z",
  "date_modified": "2026-03-02T18:00:18.518000Z",
  "file_hash": "b26cd4b3553433b1a45e8923174d0ce1b77a8d7f49718ec8bbfd1bb0163084d8",
  "private": false,
  "record": {
    "abstract": "We compute as a function of rapidity $y$ the baryon number carried by quarks\nand antiquarks with $p_T \u003e p_0 \\approx$ 2 GeV produced in Pb+Pb collisions at\nTeV energies. The computation is carried out in lowest order QCD perturbation\ntheory using structure functions compatible with HERA results. At $p_0=2$ GeV\nthe initial gluon density is both transversally saturated and thermalised in\nthe sense that the energy/gluon equals to that of an ideal gas with the same\nenergy density. Even at these high energies the initial net baryon number\ndensity at $y=0$ at $\\tau=0.1$ fm will be more than the normal nuclear matter\ndensity but the baryon-to-entropy ratio is only $(B-\\bar B)/S\\sim 1/5000$.\nFurther evolution of the system is discussed and the final baryon-to-entropy\nratio is estimated.",
    "arxiv_id": "nucl-th/9610015",
    "authors": [
      "K. J. Eskola",
      "K. Kajantie"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "journal_ref": "Z.Phys. C75 (1997) 515-522",
    "title": "Baryon-to-entropy ratio in very high energy nuclear collisions",
    "url": "https://arxiv.org/abs/nucl-th/9610015"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "c169663e-b8b8-4be4-8218-2441cfdac8a7",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}