{
  "annotation_id": "f571e95b-5ee8-48ae-b764-181ab616702c",
  "date_created": "2026-03-02T18:00:22.321000Z",
  "date_modified": "2026-03-02T18:00:22.321000Z",
  "file_hash": "4cd454b2906fc10f82052100f8b283c92792368f0da69163bb56bf6488056a9a",
  "private": false,
  "record": {
    "abstract": "The pole positions of the various baryon resonances are known to reveal\nwell-pronounced clustering, so-called Hoehler clusters. For nonstrange baryons\nthe Hoehler clusters are shown to be identical to Lorentz multiplets of the\ntype (j,j)*[(1/2,0)+(0,1/2)] with j being a half-integer. For the Lambda\nhyperons below 1800 MeV these clusters are shown to be of the type [(1,0)+\n(0,1)]*[(1/2,0)+(0,1/2)] while above 1800 MeV they are parity duplicated\n(J,0)+(0,J) (Weinberg-Ahluwalia) states. Therefore, for Lambda hyperons the\nrestoration of chiral symmetry takes place above 1800 MeV. Finally, it is\ndemonstrated that the description of spin-3/2 particles in terms of a 2nd rank\nantisymmetric Lorentz tensor with Dirac spinor components does not contain any\noff-shell parameters and avoids the main difficulties of the Rarita-Schwinger\ndescription based upon a 4-vector with Dirac spinor components.",
    "arxiv_id": "nucl-th/9712072",
    "authors": [
      "M. Kirchbach"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "doi": "10.1142/S0217732397003307",
    "journal_ref": "Mod.Phys.Lett. A12 (1997) 3177-3188",
    "title": "Lorentz Multiplet Structure of Baryon Spectra and Relativistic   Description",
    "url": "https://arxiv.org/abs/nucl-th/9712072"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "cde7fc87-c920-4592-bfdf-2db923b95c4d",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}