{
  "id": "quant-ph/0701136",
  "version": "v2",
  "published": "2007-01-19T02:32:05.000Z",
  "updated": "2009-04-29T10:37:10.000Z",
  "title": "Angular momentum of the physical electron",
  "authors": [
    "A. M. Stewart"
  ],
  "comment": "revision, 3 pages pdf",
  "journal": "Canadian Journal of Physics 87 (2) 151-152 (2009)",
  "doi": "10.1139/P08-116",
  "categories": [
    "quant-ph"
  ],
  "abstract": "The angular momentum of the physical electron, modelled as a Dirac fermion coupled to the electromagnetic field, is found to be hbar/2, the same as that of a bare Dirac fermion and independent of the size of the electric charge.",
  "revisions": [
    {
      "version": "v2",
      "updated": "2009-04-29T10:37:10.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "angular momentum",
      "physical electron",
      "bare dirac fermion",
      "electromagnetic field"
    ],
    "tags": [
      "journal article"
    ],
    "note": {
      "typesetting": "TeX",
      "pages": 3,
      "language": "en",
      "license": "arXiv",
      "status": "editable"
    }
  }
}