{
  "annotation_id": "6800a576-2506-4940-a12b-5f11e34141a6",
  "date_created": "2026-03-02T18:00:21.510000Z",
  "date_modified": "2026-03-02T18:00:21.510000Z",
  "file_hash": "fd925d9ac3e8659d02a31b8546b0f3c3241f78f9626e4decab3e0af9a0f0a544",
  "private": false,
  "record": {
    "abstract": "An attractive, energy-dependent mean-field potential for baryons is\nintroduced in order to generate a soft region in the nuclear equation-of-state,\nas suggested by recent lattice QCD calculations of baryon free matter at finite\ntemperature. Based on a hadronic transport model, we find that although this\nequation-of-state has negligible effects on the inclusive hadronic spectra, it\nleads to a minimum in the energy dependence of the transverse collective flow\nand a delayed expansion of the compressed matter. In particular, the transverse\nflow changes its direction as the colliding system passes through the softest\nregion in the equation-of-state.",
    "arxiv_id": "nucl-th/9807088",
    "authors": [
      "Bao-An Li",
      "C. M. Ko"
    ],
    "categories": [
      "nucl-th",
      "nucl-ex"
    ],
    "doi": "10.1103/PhysRevC.58.1382",
    "journal_ref": "Phys.Rev.C58:1382-1384,1998",
    "title": "Probing the softest region of nuclear equation of state",
    "url": "https://arxiv.org/abs/nucl-th/9807088"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "2da832f1-aa09-4958-91cc-8ec55b5bc7e5",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}