{
  "annotation_id": "58fb03bd-d87c-4eb2-a16a-93377ea08100",
  "date_created": "2026-03-02T18:02:13.402000Z",
  "date_modified": "2026-03-02T18:02:13.402000Z",
  "file_hash": "ec6bca58581b7ee4d503a1e17d7a88930c91329835bd3ce76a8ebd9dc8a7d3a3",
  "private": false,
  "record": {
    "abstract": "Maximally entangled states are of utmost importance to quantum communication,\ndense coding, and quantum teleportation. With a trapped ion placed inside a\nhigh finesse optical cavity, interacting with field of an external laser and\nquantized cavity field, a scheme to generate a maximally entangled three qubit\nGHZ state, is proposed. The dynamics of tripartite entanglement is\ninvestigated, using negativity as an entanglement measure and linear entropy as\na measure of mixedness of a state. It is found that (a) the number of modes\navailable to the subsystem determines the maximum entanglement of a subsystem,\nb) at entanglement maxima and minima, linear entropy and negativity uniquely\ndetermine the nature of state, but the two measures do not induce the same\nordering of states, and c) for a special choice of system parameters maximally\nentangled tripartite two mode GHZ state is generated. The scheme presented for\nGHZ state generation is a single step process and is reduction free.\n  PACS: 03.67.-a, 42.50.-p, 03.67.Dd",
    "arxiv_id": "quant-ph/0502008",
    "authors": [
      "S. Shelly Sharma",
      "N. K. Sharma"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1238/Physica.Topical.118a00272",
    "journal_ref": "Physica Scripta, T118, 272 - 275, (2005).",
    "title": "Dynamics of tripartite entanglement",
    "url": "https://arxiv.org/abs/quant-ph/0502008"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "31447df2-c1ae-463f-bb73-379009273dfe",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}