{
  "annotation_id": "a22e7db5-789e-469c-96e3-a2c754082d1e",
  "date_created": "2026-03-02T18:01:49.009000Z",
  "date_modified": "2026-03-02T18:01:49.009000Z",
  "file_hash": "511190ebabda1ee4521ad22d1ad843a1e2cae52fd33e7443ce3c6dfab336148c",
  "private": false,
  "record": {
    "abstract": "We consider the amount of work which can be extracted from a heat bath using\na bipartite state shared by two parties. In general it is less then the amount\nof work extractable when one party is in possession of the entire state. We\nderive bounds for this \"work deficit\" and calculate it explicitly for a number\nof different cases. For pure states the work deficit is exactly equal to the\ndistillable entanglement of the state, and this is also achievable for\nmaximally correlated states. In these cases a form of complementarity exists\nbetween physical work which can be extracted and distillable entanglement. The\nwork deficit is a good measure of the quantum correlations in a state and\nprovides a new paradigm for understanding quantum non-locality.",
    "arxiv_id": "quant-ph/0112074",
    "authors": [
      "Jonathan Oppenheim",
      "Michal Horodecki",
      "Pawel Horodecki",
      "Ryszard Horodecki"
    ],
    "categories": [
      "quant-ph",
      "cond-mat"
    ],
    "doi": "10.1103/PhysRevLett.89.180402",
    "journal_ref": "Phys. Rev. Lett. 89, 180402 (2002)",
    "title": "A Thermodynamical Approach to Quantifying Quantum Correlations",
    "url": "https://arxiv.org/abs/quant-ph/0112074"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "252101d2-d3e1-4a14-a17b-c16010f458e2",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}