{
  "annotation_id": "fa73374e-0523-45c0-9b44-5477684f90f0",
  "date_created": "2026-03-02T18:00:14.876000Z",
  "date_modified": "2026-03-02T18:00:14.876000Z",
  "file_hash": "95223fd48bc59beb0d7cfe6d04bc9de1c06a7031c7a2cf54816e616714423452",
  "private": false,
  "record": {
    "abstract": "The $\\gamma$-circular polarizations ($P_{\\gamma}$) and asymmetries\n($A_{\\gamma}$) of the parity forbidden M1 + E2 $\\gamma$-decays: $^{36}Cl^{\\ast}\n(J^{\\pi} = 2^{-}; T = 1; E_{x} = 1.95 $ MeV) $\\rightarrow$ $^{36}Cl (J^{\\pi} =\n2^{+}; T = 1; g.s.)$ and $^{36}Ar^{\\ast} (J^{\\pi} = 2^{-}; T = 0; E_{x} = 4.97\n$ MeV) $\\rightarrow$ $^{36}Ar^{\\ast} (J^{\\pi} = 2^{+}; T = 0; E_{x} = 1.97 $\nMeV) are investigated theoretically. We use the recently proposed\nWarburton-Becker-Brown shell-model interaction. For the weak forces we discuss\ncomparatively different weak interaction models based on different assumptions\nfor evaluating the weak meson-hadron coupling constants. The results determine\na range of $P_{\\gamma}$ values from which we find the most probable values:\n$P_{\\gamma}$ = $1.1 \\cdot 10^{-4}$ for $^{36}Cl$ and $P_{\\gamma}$ = $3.5 \\cdot\n10^{-4}$ for $^{36}Ar$.",
    "arxiv_id": "nucl-th/9410009",
    "authors": [
      "Mihai Horoi"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.50.2392",
    "journal_ref": "Phys.Rev.C50:2392-2397,1994",
    "title": "Parity Mixed Doublets in A = 36 Nuclei",
    "url": "https://arxiv.org/abs/nucl-th/9410009"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "2e81bfdb-1b4e-4f5b-af86-fb9568264ab5",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}