{
  "annotation_id": "ecbeb041-7771-488c-8058-256600326df6",
  "date_created": "2026-03-02T18:00:00.673000Z",
  "date_modified": "2026-03-02T18:00:00.673000Z",
  "file_hash": "98d1d9b60c0ac7d46b7a0a324ba437b5c1501ea4037bbf9004283e88e17a840a",
  "private": false,
  "record": {
    "abstract": "The shape of Bose-Einstein (or HBT) correlation functions is determined for\nthe case when particles are emitted from a stable source, obtained after\nconvolutions of large number of elementary random processes. The two-particle\ncorrelation function is shown to have a {\\it stretched exponential} shape,\ncharacterized by the L\\\u0027evy index of stability $ 0 \u003c \\alpha \\le 2$ and the\nscale parameter $R$. The normal, Gaussian shape corresponds to a particular\ncase, when $\\alpha = 2$ is selected. The asymmetry parameter of the stable\nsource, $\\beta$ is shown to be proportional to the angle, measured by the\nnormalized three-particle cumulant correlations.",
    "arxiv_id": "nucl-th/0402035",
    "authors": [
      "T. Csorgo",
      "S. Hegyi",
      "W. A. Zajc"
    ],
    "categories": [
      "nucl-th"
    ],
    "journal_ref": "Nukleonika 2004; 49: S7-S10",
    "title": "Stable Bose-Einstein correlations",
    "url": "https://arxiv.org/abs/nucl-th/0402035"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "b7e6ae6e-bda2-4cf2-be1e-2e4e219eb6cb",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}