{
  "annotation_id": "faf39559-9daa-4f5c-b604-5d4373cb6648",
  "date_created": "2026-03-02T18:00:11.221000Z",
  "date_modified": "2026-03-02T18:00:11.221000Z",
  "file_hash": "9c121f05f40e35f0637ef84e1836680b3c39487fce9fe2180b420457255d13ed",
  "private": false,
  "record": {
    "abstract": "Hyperon-nucleon interactions are presented that are derived either in the\nconventional meson-exchange picture or within leading order chiral effective\nfield theory. The chiral potential consists of one-pseudoscalar-meson exchanges\nand non-derivative four-baryon contact terms. With regard to meson-exchange\nhyperon-nucleon models we focus on the new potential of the Juelich group,\nwhose most salient feature is that the contributions in the scalar--isoscalar\n(\\sigma) and vector--isovector (\\rho) exchange channels are constrained by a\nmicroscopic model of correlated \\pi\\pi and KKbar exchange.",
    "arxiv_id": "nucl-th/0702015",
    "authors": [
      "J. Haidenbauer",
      "Ulf-G. Mei\u00dfner",
      "A. Nogga",
      "H. Polinder"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1007/978-3-540-72039-3_4",
    "journal_ref": "Lect.NotesPhys.724:113-140,2007",
    "title": "The hyperon-nucleon interaction: conventional versus effective field   theory approach",
    "url": "https://arxiv.org/abs/nucl-th/0702015"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "4dacbcba-5e04-453b-b7ab-eb933d0c66b6",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}