{
  "annotation_id": "1166a47d-1e18-4288-beb5-d97867810d8c",
  "date_created": "2026-03-02T18:00:25.309000Z",
  "date_modified": "2026-03-02T18:00:25.309000Z",
  "file_hash": "d4bb40a3cec81db644e2f166d0db3d07d641987202af1ad058f8ede5f00ccf4f",
  "private": false,
  "record": {
    "abstract": "Using a recently developed effective field theory for the interactions of\nnucleons at non-relativistic energies, we calculate the rate for the fusion\nprocess $p + p \\ra d + e^+ + \\nu_e$ to leading order in the momentum expansion.\nCoulomb effects are included non-perturbatively in a systematic way. The\nresulting rate is independent of specific models for the strong interactions at\nshort distances and is in agreement with the standard result in the zero-range\napproximation.",
    "arxiv_id": "nucl-th/9902064",
    "authors": [
      "Xinwei Kong",
      "Finn Ravndal"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/S0375-9474(99)00314-0",
    "journal_ref": "Nucl.Phys. A656 (1999) 421-429",
    "title": "Proton-Proton Fusion in Leading Order of Effective Field Theory",
    "url": "https://arxiv.org/abs/nucl-th/9902064"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "8643eef4-3059-4e50-9a73-bfa8f436306e",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}