{
  "annotation_id": "62f18166-1788-4606-8b96-146cfe958029",
  "date_created": "2026-03-02T18:02:41.228000Z",
  "date_modified": "2026-03-02T18:02:41.228000Z",
  "file_hash": "7c05609fa545c947b9fd2a9565ff38c88893e68e8677f6982dcabf4d21dd0ee4",
  "private": false,
  "record": {
    "abstract": "The stationary solution \\rho of a quantum master equation can be represented\nas an ensemble of pure states in a continuous infinity of ways. An ensemble\nwhich is physically realizable through monitoring the system\u0027s environment we\ncall an `unraveling\u0027. The survival probability S(t) of an unraveling is the\naverage probability for each of its elements to be unchanged a time t after\ncessation of monitoring. The maximally robust unraveling is the one for which\nS(t) remains greater than the largest eigenvalue of \\rho for the longest time.\nThe optical parametric oscillator is a soluble example.",
    "arxiv_id": "quant-ph/9709014",
    "authors": [
      "H. M. Wiseman",
      "J. A. Vaccaro"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1016/S0375-9601(98)00774-9",
    "journal_ref": "Phys.Lett. A250 (1998) 241-248",
    "title": "Maximally Robust Unravelings of Quantum Master Equations",
    "url": "https://arxiv.org/abs/quant-ph/9709014"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "e1c9bd49-ccc2-424f-812b-35dd99e1a88c",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}