{
  "annotation_id": "24e99ec5-d0aa-459b-9077-e0cd436008b6",
  "date_created": "2026-03-02T18:00:28.040000Z",
  "date_modified": "2026-03-02T18:00:28.040000Z",
  "file_hash": "a33702959629d5d106ab7e1c072746319a63c1956257ba2e4919c7e667e185f3",
  "private": false,
  "record": {
    "abstract": "Understanding an important class of experiments requires that light-front\ndynamics and related light cone variables k^+ and k_perp be used. If one uses\nk^+ as a momentum variable, the corresponding canonical spatial variable is\nx^-=x^0-x^3 and the time variable is x^0+x^3. This is the light front (LF)\napproach of Dirac. A relativistic light front formulation of nuclear dynamics\nis developed and applied to treating infinite nuclear matter in a method which\nincludes the corelations of pairs of nculeons. This is light front Brueckner\ntheory.",
    "arxiv_id": "nucl-th/9910053",
    "authors": [
      "G. A. Miller"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1142/S0217979201006021",
    "journal_ref": "Int.J.Mod.Phys.B15:1551-1557,2001",
    "title": "Infinite Nuclear Matter on the Light Front: A Modern Approach to   Brueckner Theory",
    "url": "https://arxiv.org/abs/nucl-th/9910053"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "572ce85b-5d1b-45c2-9fbd-def821d661bc",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}