{
  "annotation_id": "72d1a525-eef7-45e4-a704-e67bbb114e9b",
  "date_created": "2026-03-02T18:00:04.339000Z",
  "date_modified": "2026-03-02T18:00:04.339000Z",
  "file_hash": "38b39bfb5c7ba720d019770e498c96905fbf67c70cd540d7eeaa462ebd297fba",
  "private": false,
  "record": {
    "abstract": "We study the spin- and flavour- dependent SU(6) violations in the baryon\nspectrum by means of a G\\\"ursey Radicati mass formula. The average energy of\neach SU(6)-multiplet is described using the SU(6) invariant interaction given\nby a hypercentral potential containing a linear and a hypercoulomb term. We\nshow that the non strange and strange baryon masses are in general fairly well\nreproduced and moreover that the G\\\"ursey Radicati formula holds in a\nsatisfactory way also for the excited states up to 2 GeV. The coefficients of\nthe G\\\"ursey Radicati SU(6) breaking part obtained by the fit of the\nthree-quark spectrum can be used to evaluate in first approximation the\nsplitting within multiplets also for exotic baryon systems.",
    "arxiv_id": "nucl-th/0506032",
    "authors": [
      "M. M. Giannini E. Santopinto",
      "A. Vassallo"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "doi": "10.1140/epja/i2005-10113-4",
    "journal_ref": "Eur.Phys.J. A25 (2005) 241-247",
    "title": "A New Application of the Gursey and Radicati Mass Formula",
    "url": "https://arxiv.org/abs/nucl-th/0506032"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "0e545095-80a3-404e-a694-a3358c53cd42",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}