{
  "id": "nucl-th/9505044",
  "version": "v1",
  "published": "1995-05-29T04:47:57.000Z",
  "updated": "1995-05-29T04:47:57.000Z",
  "title": "Strangelets at finite temperature",
  "authors": [
    "M. G. Mustafa",
    "A. Ansari"
  ],
  "comment": "Revtex file+4 figures(ps files)",
  "journal": "Phys.Rev.D53:5136,1996; Erratum-ibid.D54:4694,1996",
  "doi": "10.1103/PhysRevD.53.5136 10.1103/PhysRevD.54.4694",
  "categories": [
    "nucl-th"
  ],
  "abstract": "Within the MIT bag model picture of QCD, we have studied the stability of finite size strangelets at finite temperature with baryon number $A \\leq 100$. The light quarks $u$ and $d$ are considered massless while mass of the $s$ quark is taken as $150$ MeV. Using discrete eigen energies of the non-interacting quarks in the bag, grand canonical partition function is constructed and then the free energy is minimized with respect to the bag radius. In the $T\\rightarrow 0$ limit clear shell structures are found which persist upto about $T=10$ MeV. Infact for $A=6$ the shell structure disappears only at $T > 20$ MeV.",
  "revisions": [
    {
      "version": "v1",
      "updated": "1995-05-29T04:47:57.000Z"
    }
  ],
  "analyses": {
    "subjects": [
      "24.85.+p",
      "12.39.Ba",
      "12.38.Mh"
    ],
    "keywords": [
      "finite temperature",
      "strangelets",
      "limit clear shell structures",
      "mit bag model picture",
      "grand canonical partition function"
    ],
    "tags": [
      "journal article"
    ],
    "publication": {
      "publisher": "APS",
      "journal": "Phys. Rev. D"
    },
    "note": {
      "typesetting": "RevTeX",
      "pages": 0,
      "language": "en",
      "license": "arXiv",
      "status": "editable",
      "inspire": 395710
    }
  }
}