{
  "annotation_id": "209c16e1-392e-4614-97dc-7eee74f58e47",
  "date_created": "2026-03-02T18:00:45.832000Z",
  "date_modified": "2026-03-02T18:00:45.832000Z",
  "file_hash": "9350a0343a51ecb6855e6b0215e64efd1a83bd07ef0681012c098c6a60ae2bc4",
  "private": false,
  "record": {
    "abstract": "The Coulomb-gauge vector potential of a uniformly moving point charge is\nobtained by calculating the gauge function for the transformation between the\nLorenz and Coulomb gauges. The expression obtained for the difference between\nthe vector potentials in the two gauges is shown to satisfy a Poisson equation\nto which the inhomogeneous wave equation for this quantity can be reduced. The\nright-hand side of the Poisson equation involves an important but easily\noverlooked delta-function term that arises from a second-order partial\nderivative of the Coulomb potential of a point charge.",
    "arxiv_id": "physics/0307124",
    "authors": [
      "V. Hnizdo"
    ],
    "categories": [
      "physics.class-ph",
      "physics.gen-ph"
    ],
    "journal_ref": "Eur. J. Phys. vol. 25, 351--360 (2004)",
    "title": "Potentials of a uniformly moving point charge in the Coulomb gauge",
    "url": "https://arxiv.org/abs/physics/0307124"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "54c665ee-9af3-41a4-98a1-261faf0cb2bb",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}