{
  "annotation_id": "a6f28330-748a-44d3-bf34-f98a926d854e",
  "date_created": "2026-03-02T18:00:14.938000Z",
  "date_modified": "2026-03-02T18:00:14.938000Z",
  "file_hash": "2dc52f22a23f082bb937cf2e78fb1762335bfd02cf6262cf3bbf50ba8f4c32c8",
  "private": false,
  "record": {
    "abstract": "Using a three-baryon $\\Lambda NN$ potential having a spin-independent\ndispersive and a two-pion exchange components, realistic variational Monte\nCarlo calculations have been performed for the $\\Lambda$-seperation energy for\n$^{5}_{\\Lambda}$He. A relationship between strengths associated with both\npieces of $\\Lambda NN$ force giving exact experimental $\\Lambda$-seperation\nenergy has been obtained which then combined with our previous study on\n$^{17}_{\\,\\,\\Lambda}$O hypernucleus determines a unique and acceptable set of\nstrength parameters for $\\Lambda NN$ potential. The $\\Lambda NN$ force is found\nimportant for the core polarization.",
    "arxiv_id": "nucl-th/9503023",
    "authors": [
      "A. A. Usmani"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.52.1773",
    "journal_ref": "Phys.Rev.C52:1773-1777,1995",
    "title": "The three-baryon $\\Lambda NN$ potential",
    "url": "https://arxiv.org/abs/nucl-th/9503023"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "082a9b44-6d0c-423f-863d-6c103ac2014b",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}