{
  "annotation_id": "1577bf33-0ca4-4e09-8538-ba5842d9f812",
  "date_created": "2026-03-02T18:00:43.126000Z",
  "date_modified": "2026-03-02T18:00:43.126000Z",
  "file_hash": "4223841c771d4dd648492d67ab828b9854058d39187d18b5b7ae9aad8572770d",
  "private": false,
  "record": {
    "abstract": "We define and compute the renormalized four-momentum of the composed physical\nsystem: classical Maxwell field interacting with charged point particles. As a\n`reference\u0027 configuration for the field surrounding the particle, we take the\nBorn solution. Unlike in the previous approach [Gen. Relat. Grav. 26 (1994)\n167; Acta Phys. Pol. A 85 (1994) 771; Commun. Math. Phys. 198 (1998), 711],\nbased on the Coulomb `reference\u0027, a dependence of the four-momentum of the\nparticle (`dressed\u0027 with the Born solution) upon its acceleration arises in a\nnatural way. This will change the resulting equations of motion. Similarly, we\ntreat the angular momentum tensor of the system.",
    "arxiv_id": "physics/0304056",
    "authors": [
      "J. Kijowski",
      "P. Podles"
    ],
    "categories": [
      "physics.class-ph"
    ],
    "doi": "10.1016/S0393-0440(03)00049-4",
    "journal_ref": "J. Geom. Phys. 48 (2003), 369-384",
    "title": "Born renormalization in classical Maxwell electrodynamics",
    "url": "https://arxiv.org/abs/physics/0304056"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "1a0329bb-d7cc-4dcf-b141-6f119afe48f8",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}