{
  "annotation_id": "79b52ce4-4f4e-41fe-92f0-5e1079c0a78c",
  "date_created": "2026-03-02T18:00:15.350000Z",
  "date_modified": "2026-03-02T18:00:15.350000Z",
  "file_hash": "79e9ecf63a682eb28990d33b51968d00f241fc5a6f464294f7e782bb4b640703",
  "private": false,
  "record": {
    "abstract": "Mass of a baryon as a function of temperature is calculated using\ncolour-singlet partition function for massless quarks (with two flavours) and\nabelian gluons confined in a bag with a temperature dependent bag pressure\nconstant $B(T)$. The non-perturbative aspect of QCD interaction is included\nthrough colour-singlet restriction on quark-gluon partition function in a\nphenomenological way. The entropy bound inequality $ S/E \\ \\leq \\ 2\\pi R/\\hbar\nc $, where $S, \\ E $ and $R$ are entropy, energy and radius, respectively of\nthe enclosed system with $\\hbar c \\ = \\ 197.331 $ MeVfm, is found to be\nconsistent with the equilibrium solutions of the baryon mass upto a temperature\n$T_E$. There is a region of temperature $T_E \u003c T \u003c T_C$ ($T_C$ is critical\ntemperature for quark-gluon plasma formation) in which no admissible\nequilibrium states exist for the bag. We say that the system expriences a phase\njump from hadron to quark-gluon plasma through thermodynamic non-equlibrium\nprocesses.",
    "arxiv_id": "nucl-th/9505041",
    "authors": [
      "M. G. Mustafa",
      "A. Ansari"
    ],
    "categories": [
      "nucl-th"
    ],
    "title": "Temperature dependent Nucleon Mass and entropy bound inequality",
    "url": "https://arxiv.org/abs/nucl-th/9505041"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "9923bd5c-a00f-40f5-94cb-c94ae06c8c4b",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}