{
  "annotation_id": "76205bdd-4f32-4f0d-aa83-926f465a5ffa",
  "date_created": "2026-03-02T18:00:14.924000Z",
  "date_modified": "2026-03-02T18:00:14.924000Z",
  "file_hash": "60b207ebe287e39c8a10dc02fd7e98ca065d6af84f89b953410fb6ce2cfff4b0",
  "private": false,
  "record": {
    "abstract": "Within the MIT bag model picture of QCD, we have studied the stability of\nfinite size strangelets at finite temperature with baryon number $A \\leq 100$.\nThe light quarks $u$ and $d$ are considered massless while mass of the $s$\nquark is taken as $150$ MeV. Using discrete eigen energies of the\nnon-interacting quarks in the bag, grand canonical partition function is\nconstructed and then the free energy is minimized with respect to the bag\nradius. In the $T\\rightarrow 0$ limit clear shell structures are found which\npersist upto about $T=10$ MeV. Infact for $A=6$ the shell structure disappears\nonly at $T \u003e 20$ MeV.",
    "arxiv_id": "nucl-th/9505044",
    "authors": [
      "M. G. Mustafa",
      "A. Ansari"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevD.53.5136 10.1103/PhysRevD.54.4694",
    "journal_ref": "Phys.Rev.D53:5136,1996; Erratum-ibid.D54:4694,1996;\n  Phys.Rev.D54:4694,1996",
    "title": "Strangelets at finite temperature",
    "url": "https://arxiv.org/abs/nucl-th/9505044"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "61b1ff13-2e53-4b64-937c-bbf6ad21e957",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}