{
  "annotation_id": "369724d9-546c-4049-88fd-7384754328ba",
  "date_created": "2026-03-02T18:00:05.083000Z",
  "date_modified": "2026-03-02T18:00:05.083000Z",
  "file_hash": "f3ae97202be87b39f79e303a8e046aa0d5d39cbafe8b56d96db71bc33d6b7d4a",
  "private": false,
  "record": {
    "abstract": "We study the triton and three-nucleon force at lowest chiral order in\npionless effective field theory both in the Hamiltonian and Euclidean nuclear\nlattice formalism. In the case of the Euclidean lattice formalism, we derive\nthe exact few-body worldline amplitudes corresponding to the standard many-body\nlattice action. This will be useful for setting low-energy coefficients in\nfuture nuclear lattice simulations. We work in the Wigner SU(4)-symmetric limit\nwhere the S-wave scattering lengths {1}S{0} and {3}S{1} are equal. By comparing\nwith continuum results, we demonstrate for the first time that the nuclear\nlattice formalism can be used to study few-body nucleon systems.",
    "arxiv_id": "nucl-th/0510047",
    "authors": [
      "B. Borasoy",
      "H. Krebs",
      "D. Lee",
      "U. -G. Mei\u00dfner"
    ],
    "categories": [
      "nucl-th",
      "hep-lat",
      "hep-ph"
    ],
    "doi": "10.1016/j.nuclphysa.2006.01.009",
    "journal_ref": "Nucl.Phys. A768 (2006) 179-193",
    "title": "The triton and three-nucleon force in nuclear lattice simulations",
    "url": "https://arxiv.org/abs/nucl-th/0510047"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "e86165de-3f9b-4011-8e7e-45b8c8f72148",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}