{
  "annotation_id": "d75fe68a-e3c6-4755-9bfd-50fbda5b1c6b",
  "date_created": "2026-03-02T18:00:28.795000Z",
  "date_modified": "2026-03-02T18:00:28.795000Z",
  "file_hash": "511caf26bc026386e6a140894bd390700c5387b511974f952747dd6ca72245b3",
  "private": false,
  "record": {
    "abstract": "We calculate in (two-loop) chiral perturbation theory the local NN-potentials\ngenerated by the three-pion exchange diagrams proportional to g_A^4 and g_A^6.\nSurprisingly, we find that the total isoscalar central $3\\pi$-exchange\npotential vanishes identically. The individually largest $3\\pi$-exchange\npotentials are of isoscalar spin-spin, isovector central and isoscalar tensor\ntype. For these potentials simple analytical expressions can be given. The\nstrength of these dominant $3\\pi$-exchange potentials at r=1.0 fm is 4.6 MeV,\n2.9 MeV and 1.4 MeV, respectively. Furthermore, we observe that the spin-spin\nand tensor potentials due to the diagrams proportional to g_A^6 do not exist in\nthe infinite nucleon mass limit.",
    "arxiv_id": "nucl-th/9912054",
    "authors": [
      "N. Kaiser"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.62.024001",
    "journal_ref": "Phys.Rev. C62 (2000) 024001",
    "title": "Chiral $\\pi$-exchange NN-potentials: Results for diagrams proportional   to g_A^4 and g_A^6",
    "url": "https://arxiv.org/abs/nucl-th/9912054"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "2352101e-89f1-4cda-9915-2871003ea461",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}