{
  "annotation_id": "dc126477-9083-4c89-9d55-4826d95999f4",
  "date_created": "2026-03-02T18:02:45.029000Z",
  "date_modified": "2026-03-02T18:02:45.029000Z",
  "file_hash": "5992ca2eb749b17a33d2bc6723a13487eb5fc26bfacdbe7fbd76cdf3a3739fdb",
  "private": false,
  "record": {
    "abstract": "A complete thermodynamic treatment of the Casimir effect is presented.\nExplicit expressions for the free and the internal energy, the entropy and the\npressure are discussed. As an example we consider the Casimir effect with\ndifferent temperatures between the plates ($T$) resp. outside of them ($T\u0027$).\nFor $T\u0027\u003cT$ the pressure of heat radiation can eventually compensate the Casimir\nforce and the total pressure can vanish. We consider both an isothermal and an\nadiabatic treatment of the interior region. The equilibrium point (vanishing\npressure) turns out instable in the isothermal case. In the adiabatic situation\nwe have both an instable and a stable equilibrium point, if $T\u0027/T$ is\nsufficiently small. Quantitative aspects are briefly discussed.",
    "arxiv_id": "quant-ph/9902074",
    "authors": [
      "H. Mitter",
      "D. Robaschik"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1007/s100510050039",
    "journal_ref": "Eur.Phys.J.B13:335-340,2000",
    "title": "Thermodynamics of the Casimir effect",
    "url": "https://arxiv.org/abs/quant-ph/9902074"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "cf5ec219-5945-4612-b688-60dcae03d1c7",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}