{
  "annotation_id": "2e8ce92c-2482-42c9-b50b-2344de5840a3",
  "date_created": "2026-03-02T18:02:34.321000Z",
  "date_modified": "2026-03-02T18:02:34.321000Z",
  "file_hash": "cc6f93b31f96be8a9cec1e9db498f27328a5790d282d043dd2d3981349e5c80b",
  "private": false,
  "record": {
    "abstract": "The transition from classical to quantum behavior for chaotic systems is\nunderstood to be accompanied by the suppression of chaotic effects as the\nrelative size of $\\hbar$ is increased. We show evidence to the contrary in the\nbehavior of the quantum trajectory dynamics of a dissipative quantum chaotic\nsystem, the double-well Duffing oscillator. The classical limit in the case\nconsidered has regular behavior, but as the effective $\\hbar$ is increased we\nsee chaotic behavior. This chaos then disappears deeper into the quantum\nregime, which means that the quantum-classical transition in this case is\nnon-monotonic in $\\hbar$.",
    "arxiv_id": "quant-ph/0702174",
    "authors": [
      "Arie Kapulkin",
      "Arjendu K. Pattanayak"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1103/PhysRevLett.101.074101",
    "title": "Non-monotonicity in the quantum-classical transition: Chaos induced by   quantum effects",
    "url": "https://arxiv.org/abs/quant-ph/0702174"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "0bd8fd93-1b4a-4261-8492-247e5096e02f",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}