{
  "annotation_id": "db2f814f-fc84-4602-93f4-9593f60356e3",
  "date_created": "2026-03-02T18:01:56.063000Z",
  "date_modified": "2026-03-02T18:01:56.063000Z",
  "file_hash": "eec2b985f9d14a4051ee434cf461a08c145275ba428b805f906b3b8226991977",
  "private": false,
  "record": {
    "abstract": "Quantum compression can be thought of not only as compression of a signal,\nbut also as a form of cooling. In this view, one is interested not in the\nsignal, but in obtaining purity. In compound systems, one may be interested to\ncool the system to obtain {\\it local purity} by use of local operations and\nclassical communication [Oppenheim et al. Phys. Rev. Lett. 89,180402 (2002)].\nHere we compare it with usual compression and find that it can be represented\nas compression with suitably restricted means.",
    "arxiv_id": "quant-ph/0302139",
    "authors": [
      "Michal Horodecki",
      "Pawel Horodecki",
      "Jonathan Oppenheim"
    ],
    "categories": [
      "quant-ph"
    ],
    "title": "Compressing compound states",
    "url": "https://arxiv.org/abs/quant-ph/0302139"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "62a3274e-64d4-45d4-bde2-58ee61b39df0",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}