{
  "annotation_id": "898012da-1b2f-43d7-963f-f3bd988e280e",
  "date_created": "2026-03-02T18:01:18.019000Z",
  "date_modified": "2026-03-02T18:01:18.019000Z",
  "file_hash": "c8318440544447b7036a68193053c034f83765e245cae2912943be31d643d221",
  "private": false,
  "record": {
    "abstract": "Dirac matrices, also known as gamma matrices, are defined only up to a\nsimilarity transformation. Usually, some explicit representation of these\nmatrices is assumed in order to deal with them. In this article, we show how it\nis possible to proceed without any such assumption. Various important\nidentities involving Dirac matrices and spinors have been derived without\nassuming any representation at any stage.",
    "arxiv_id": "physics/0703214",
    "authors": [
      "Palash B. Pal"
    ],
    "categories": [
      "physics.ed-ph",
      "hep-ph",
      "hep-th"
    ],
    "license": "http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
    "title": "Representation-independent manipulations with Dirac matrices and spinors",
    "url": "https://arxiv.org/abs/physics/0703214"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "b862c5f5-28e5-4347-ad3c-0c541961dadc",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}