{
  "annotation_id": "a5804527-be81-45cc-9d8d-2c597ebf5f43",
  "date_created": "2026-03-02T18:00:15.346000Z",
  "date_modified": "2026-03-02T18:00:15.346000Z",
  "file_hash": "e4a918255c00fce5b00cc39427c544862622de4afd0dfc7938d7b3a837e87121",
  "private": false,
  "record": {
    "abstract": "The reaction rate of the nuclear fusion d+Li6 ----\u003e Be8*(2+,0) is estimated\nin the case where the nuclei are confined to each other by a muon. For the\ndescription of nuclear transitions, a method which is analogous to the Linear\nCombination of Atomic Orbitals has been used. Using the complex coordinate\nrotation method, we found that a molecular d-mu-Li6 state exists with energy\n(-20.3084-i0.0066) eV and |\\Psi_{m}(0)|=0.44x10^{-7} fm^-3/2. The nuclear wave\nfunctions needed, were constructed in the form of antisymmetrized products of\nharmonic-oscillator functions for the three-cluster approximation, (dd\\alpha),\nto the five-body (NNNN\\alpha) problem. It was found that the reaction rate\n\\lambda is strongly dependent on the energy gap between the d-Li6 threshold and\nthe energy of the final Be8^* resonant state. The value of \\lambda obtained by\naveraging over the width of this resonance, is 0.183x10^10 sec^{-1}.",
    "arxiv_id": "nucl-th/9505039",
    "authors": [
      "S. A. Rakityansky",
      "S. A. Sofianos",
      "V. B. Belyaev",
      "V. I. Korobov"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevA.54.1242",
    "title": "Resonant nuclear transition in the d-mu-Li6 muonic molecule",
    "url": "https://arxiv.org/abs/nucl-th/9505039"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "eaf0f585-1258-4f38-9de6-2d32598cac55",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}