{
  "annotation_id": "73707924-8166-40e4-bef6-bd45065ad438",
  "date_created": "2026-03-02T18:00:25.705000Z",
  "date_modified": "2026-03-02T18:00:25.705000Z",
  "file_hash": "0fb9a2bb2d39decaa186c9f83ed6bdf91cbc55ea01c65790757d5887f3245a87",
  "private": false,
  "record": {
    "abstract": "In Faddeev calculations of ^3Hwe study the dependence of the binding on the\nthree nucleon force. We adopt the 2 pi -exchange Tucson-Melbourne three-nucleon\nforce and investigate phenomenologically the dependence on the strength of the\nindividual three-body force operators (a -, b -, c - and d -terms). While the a\n-term provides a tiny contribution the b - and d -terms provides a tiny\ncontribution the b - and d -terms are important to gain the experimental\nbinding energy. We find two solutions for the c -term, one around the value\nused in the Tucson-Melbourne model and a new one close to zero, which supports\nthe recentrecommendation of chiral perturbation theory that the short-range c\n-term should be dropped.",
    "arxiv_id": "nucl-th/9904060",
    "authors": [
      "H. Kamada",
      "D. Hueber",
      "A. Nogga"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1007/s006010170021",
    "journal_ref": "Few Body Syst. 30 (2001) 121-129",
    "title": "The c-term of the TM 3-body Force: to be or not to be",
    "url": "https://arxiv.org/abs/nucl-th/9904060"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "11b75c4d-5270-4e16-b309-ccdfb082bcf5",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}