{
  "annotation_id": "56a676d8-4124-4f18-b3e0-e39cbfac00d0",
  "date_created": "2026-03-02T18:00:08.531000Z",
  "date_modified": "2026-03-02T18:00:08.531000Z",
  "file_hash": "9157609ec23c3b22c8516deaf759e8a932d8cc83712ec679bcfb0485abab747f",
  "private": false,
  "record": {
    "abstract": "The structures of $N\\Omega_{(2,1/2)}$ and $\\Delta\\Omega_{(3,3/2)}$ with\nstrangeness $s=-3$ are dynamically studied in both the chiral SU(3) quark model\nand the extended chiral SU(3) quark model by solving a resonating group method\n(RGM) equation. The first model parameters are taken from our previous work,\nwhich gave a satisfactory description of the energies of the baryon ground\nstates, the binding energy of the deuteron, the nucleon-nucleon(NN) scattering\nphase shifts, and the hyperon-nucleon (YN) cross sections. The effect from the\nvector meson fields is very similar to that from the one-gluon exchange\ninteraction, both in the chiral SU(3) quark model and the extended chiral SU(3)\nquark model, the $N\\Omega_{(2,1/2)}$ and $\\Delta\\Omega_{(3,3/2)}$ systems are\nwealy bound states. The second model parameters are also taken from our\nprevious work by fitting the KN scattering process. when the mixing of scalar\nmesons are considered, the $N\\Omega_{(2,1/2)}$ and $\\Delta\\Omega_{(3,3/2)}$\nsystems change into unbound state.",
    "arxiv_id": "nucl-th/0606056",
    "authors": [
      "Dai Lian-Rong",
      "Zhang Dan",
      "Li Chun-Ran",
      "Tong Lei"
    ],
    "categories": [
      "nucl-th"
    ],
    "title": "Strangeness s = -3 dibaryons in a chiral quark model",
    "url": "https://arxiv.org/abs/nucl-th/0606056"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "587d6216-f0d0-4d87-acba-b873982556c5",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}