{
  "annotation_id": "3602d627-b81d-453e-99a7-346ceefefea8",
  "date_created": "2026-03-02T18:00:18.955000Z",
  "date_modified": "2026-03-02T18:00:18.955000Z",
  "file_hash": "e3ef76e826f615011af22b90dafc9597b175bf9b4418097e4d235cc597cfe3ba",
  "private": false,
  "record": {
    "abstract": "Considering the confinement of massless $u$ and $d$ quarks and massive $s$\nquarks in an axially symmetric quadrupole shaped deformable bag, the stability\nproperties of color-singlet strangelets at finite temperatures are studied for\nthe baryon number $A \\leq$ 100. It is found that, in general, at each $A$ the\nenergy of the strangelet is the lowest for the spherical shape. However, it is\ninteresting to find shell structures for the deformed shapes at some new $A$\nvalues, not found for the spherical shape. This should be of relevance for the\nexperimental search of strangelets. The color projected (singlet) calculation\nshows that even for the deformed shapes the shell structures vanish only for\nthe temperature, $T \\ga$ 30 MeV. On the other hand, from a somewhat crude\nestimate we also find that at a fixed entropy per baryon (instead of a fixed\ntemperature) of the order of unity or higher these shell structures disappear.",
    "arxiv_id": "nucl-th/9706007",
    "authors": [
      "Munshi Golam Mustafa",
      "A. Ansari"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.56.420",
    "journal_ref": "Phys.Rev.C56:420-425,1997",
    "title": "Deformed Strangelets at Finite Temperature",
    "url": "https://arxiv.org/abs/nucl-th/9706007"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "ed59f8f3-a315-4d88-9b7d-5cb761f4b179",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}