{
  "annotation_id": "d3e28899-e74d-480b-95df-6745a304abc7",
  "date_created": "2026-03-02T18:01:04.408000Z",
  "date_modified": "2026-03-02T18:01:04.408000Z",
  "file_hash": "761a712994b82539166408a0ba21c522e3a6d1ba19e83849d3d4170430a36839",
  "private": false,
  "record": {
    "abstract": "We discuss the origin of the Schott energy in the Abraham-Lorentz version of\nelectrodynamic radiation theory and how it can be used to explain some apparent\nparadoxes. We also derive the generalization of this quantity for the\nFord-O\u0027Connell equation, which has the merit of being derived exactly from a\nmicroscopic Hamiltonian for an electron with structure and has been shown to be\nfree of the problems associated with the Abraham-Lorentz theory. We emphasize\nthat the instantaneous power supplied by the applied force not only gives rise\nto radiation (acceleration fields), but it can change the kinetic energy of the\nelectron and change the Schott energy of the velocity fields. The important\nrole played by boundary conditions is noted.",
    "arxiv_id": "physics/0601170",
    "authors": [
      "Jose A. Heras",
      "R. F. O\u0027Connell"
    ],
    "categories": [
      "physics.optics",
      "physics.gen-ph",
      "quant-ph"
    ],
    "doi": "10.1119/1.2142753",
    "journal_ref": "Am. J. Phys. 74, 150 (2006)",
    "title": "Generalization of the Schott energy in electrodynamic radiation theory",
    "url": "https://arxiv.org/abs/physics/0601170"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "fe4fc7ea-7462-4292-afd8-22fac338fd6b",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}