{
  "annotation_id": "af383c18-3ff8-4598-bbed-891556e67a5e",
  "date_created": "2026-03-02T18:01:45.846000Z",
  "date_modified": "2026-03-02T18:01:45.846000Z",
  "file_hash": "f37c0253cec3711da90b82eaaf13eeae048aeb320b23103f084893be88ce2439",
  "private": false,
  "record": {
    "abstract": "We complete our previous(1, 2) demonstration that there is a family of new\nsolutions to the photon and Dirac equations using spatial and temporal circles\nand four-vector behaviour of the Dirac bispinor. We analyse one solution for a\nbound state, which is equivalent to the attractive two-body interaction between\na charged point particle and a second, which remains at rest. We show this\nyields energy and angular momentum eigenvalues that are identical to those\nfound by the usual method of solving of the Dirac equation,(4) including fine\nstructure. We complete our previous derivation(3) of QED from a set of rules\nfor the two-body interaction and generalise these. We show that QED may be\ndecomposed into a two-body interaction at every point in spacetime.",
    "arxiv_id": "quant-ph/0110162",
    "authors": [
      "Sarah B. M. Bell",
      "John P. Cullerne",
      "Bernard M. Diaz"
    ],
    "categories": [
      "quant-ph"
    ],
    "journal_ref": "FOUND.PHYS.34(2),FEB.2004",
    "title": "The two-body interaction with a circle in time",
    "url": "https://arxiv.org/abs/quant-ph/0110162"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "ca285272-8e66-48cc-a67f-341c24f0aeba",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}