{
  "id": "hep-th/9604148",
  "version": "v1",
  "published": "1996-04-23T23:38:08.000Z",
  "updated": "1996-04-23T23:38:08.000Z",
  "title": "About the Claimed Longitudinal Nature of the Antisymmetric Tensor Field After Quantization",
  "authors": [
    "Valeri V. Dvoeglazov"
  ],
  "comment": "ReVTeX file. 9pp",
  "journal": "\"Electromagnetic Phenomena\", v. 1, No. 4, pp. 465-470 (1998)",
  "categories": [
    "hep-th"
  ],
  "abstract": "It has long been claimed that antisymmetric tensor field of the second rank is longitudinal after quantization. Such a situation is quite unacceptable from a viewpoint of the Correspondence Principle. On the basis of the Lagrangian formalism we calculate the Pauli-Lyuban'sky vector of relativistic spin for this field. Even at the classical level it can be equal to zero after application of the well-known constraints. The correct quantization procedure permits us to propose solution of this puzzle in the modern field theory. Obtained results develop the previous consideration of Evans [{\\it Physica A}214 (1995) 605-618].",
  "revisions": [
    {
      "version": "v1",
      "updated": "1996-04-23T23:38:08.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "antisymmetric tensor field",
      "claimed longitudinal nature",
      "correct quantization procedure permits",
      "second rank",
      "relativistic spin"
    ],
    "tags": [
      "journal article"
    ],
    "note": {
      "typesetting": "RevTeX",
      "pages": 9,
      "language": "en",
      "license": "arXiv",
      "status": "editable",
      "inspire": 417943,
      "adsabs": "1996hep.th....4148D"
    }
  }
}