{
  "annotation_id": "86bbcb8a-8804-44fc-8c78-142648a9c0e5",
  "date_created": "2026-03-02T18:00:01.595000Z",
  "date_modified": "2026-03-02T18:00:01.595000Z",
  "file_hash": "dfb61e27b42853125066ddbe3292376bfd16c71b3f12ccc9e487ba99e10a453f",
  "private": false,
  "record": {
    "abstract": "Schiff moments were calculated for a set of nuclei with full account of core\npolarization effects. A finite range P and T violating weak nucleon-nucleon\ninteraction has been used in the calculations. While in the absence of core\npolarization the Schiff moment depends on one combination of the weak\ninteraction constants, in the presence of core polarization the Schiff moment\ndepends on all three constants separately. The dominant contribution comes from\nisovector, $\\Delta T=1$, part of the weak interaction. The effects of core\npolarization were found to have in general a large effect on the Schiff\nmoments.",
    "arxiv_id": "nucl-th/0408065",
    "authors": [
      "V. F. Dmitriev",
      "R. A. Sen\u0027kov",
      "N. Auerbach"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.71.035501",
    "journal_ref": "Phys.Rev. C71 (2005) 035501",
    "title": "Effects of core polarization on the nuclear Schiff moment",
    "url": "https://arxiv.org/abs/nucl-th/0408065"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "75251e32-173a-4ef2-ad14-eb288c7e0a23",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}