{
  "annotation_id": "19767244-6943-4395-b2e6-a6b3394f7851",
  "date_created": "2026-03-02T18:02:13.519000Z",
  "date_modified": "2026-03-02T18:02:13.519000Z",
  "file_hash": "0e75e612f0c050ce92a33d2ed74e337af78d2e0ca640910dd331db75f08b78f3",
  "private": false,
  "record": {
    "abstract": "On the basis of the relativistic symmetry of Minkowski space, we derive a\nLorentz invariant equation for a spread electron. This equation slightly\ndiffers from the Dirac equation and includes additional terms originating from\nthe spread of an electron. Further, we calculate the anomalous magnetic moment\nbased on these terms. These calculations do not include any divergence;\ntherefore, renormalization procedures are unnecessary. In addition, the\nrelativistic symmetry existing among coordinate systems will provide a new\nprospect for the foundations of quantum mechanics like the measurement process.",
    "arxiv_id": "quant-ph/0501185",
    "authors": [
      "T. Kawahara"
    ],
    "categories": [
      "quant-ph"
    ],
    "journal_ref": "EJTP 4, No. 15 (2007) 37-52",
    "title": "Considering relativistic symmetry as the first principle of quantum   mechanics",
    "url": "https://arxiv.org/abs/quant-ph/0501185"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "06a96dfb-7355-434c-8bdd-e6c6dca2250e",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}