{
  "annotation_id": "2c2c9379-a743-4e38-b2f1-3d5b881d36a7",
  "date_created": "2026-03-02T18:00:25.528000Z",
  "date_modified": "2026-03-02T18:00:25.528000Z",
  "file_hash": "f109875bb7603fc51ffd5aea30daca21b4f149c5529a08da6525a7258641ce7f",
  "private": false,
  "record": {
    "abstract": "The wave function in relativity is defined, in four-dimensional space, on a\nspace-like three-dimensional plane. The plane, most close to the time-like\nregion, is the light-front plane $ct+z=0$. Corresponding dynamical approach -\nthe light-front dynamics - has considerable advantages. We describe, in a\nfield-theoretical framework, the construction of light-front dynamics and\nillustrate it by some examples.",
    "arxiv_id": "nucl-th/9907037",
    "authors": [
      "V. A. Karmanov"
    ],
    "categories": [
      "nucl-th",
      "hep-ph",
      "hep-th"
    ],
    "title": "Light-Front Dynamics",
    "url": "https://arxiv.org/abs/nucl-th/9907037"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "46873ad2-348c-4798-99d2-4397528866f8",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}