{
  "annotation_id": "9f503c24-f062-45d8-a55c-ee2ffb175be3",
  "date_created": "2026-03-02T18:02:48.107000Z",
  "date_modified": "2026-03-02T18:02:48.107000Z",
  "file_hash": "7faa5c06364a736d9357e1472dc7e4fc86c094946691acbac0fdfc35b3db7237",
  "private": false,
  "record": {
    "abstract": "Extensions of average Hamiltonian theory to quantum computation permit the\ndesign of arbitrary Hamiltonians, allowing rotations throughout a large Hilbert\nspace. In this way, the kinematics and dynamics of any quantum system may be\nsimulated by a quantum computer. A basis mapping between the systems dictates\nthe average Hamiltonian in the quantum computer needed to implement the desired\nHamiltonian in the simulated system. The flexibility of the procedure is\nillustrated with NMR on 13-C labelled Alanine by creating the non-physical\nHamiltonian ZZZ corresponding to a three body interaction.",
    "arxiv_id": "quant-ph/9908012",
    "authors": [
      "C. H. Tseng",
      "S. Somaroo",
      "Y. Sharf",
      "E. Knill",
      "R. Laflamme",
      "T. F. Havel",
      "D. G. Cory"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1103/PhysRevA.61.012302",
    "title": "Quantum simulation of a three-body interaction Hamiltonian on an NMR   quantum computer",
    "url": "https://arxiv.org/abs/quant-ph/9908012"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "708236b3-e8c5-4fe9-9d15-ac413a3809a1",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}