{
  "annotation_id": "e96ecd0a-3c43-4e5e-9f11-cbd155a8ef10",
  "date_created": "2026-03-02T18:00:50.253000Z",
  "date_modified": "2026-03-02T18:00:50.253000Z",
  "file_hash": "7c5869be87a9bd6135b57b31b4c78c6e56b2656851b87883263f9fcb737c7269",
  "private": false,
  "record": {
    "abstract": "We suggest to use insulating garnets doped by rare earth ions for\nmeasurements of nuclear anapole moments. A parity violating shift of the NMR\nfrequency arises due to the combined effect of the lattice crystal field and\nthe anapole moment of the rare-earth nucleus.\n  We show that there are two different observable effects related to frequency:\n1) A shift of the NMR frequency in an external electric field applied to the\nsolid. The value of the shift is about \\Delta \\nu_1 ~ 10^{-5} Hz with E = 10\nkV/cm; 2) A splitting of the NMR line into two lines. The second effect is\nindependent of the external electric field. The value of the splitting is about\n\\Delta \\nu_2 ~ 0.5 Hz and it depends on the orientation of the crystal with\nrespect to magnetic field. Both estimates are presented for a magnetic field of\nabout 10 tesla.\n  We also discuss a radiofrequency electric field and a static macroscopic\nmagnetization caused by the nuclear anapole moment.",
    "arxiv_id": "physics/0405043",
    "authors": [
      "T. N. Mukhamedjanov",
      "O. P. Sushkov",
      "J. M. Cadogan"
    ],
    "categories": [
      "physics.atom-ph",
      "cond-mat.other",
      "hep-ph"
    ],
    "doi": "10.1103/PhysRevA.71.012107",
    "title": "Manifestations of nuclear anapole moments in solid state NMR",
    "url": "https://arxiv.org/abs/physics/0405043"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "73e05193-44c9-47cf-91dd-3c5d6afca3b5",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}