{
  "annotation_id": "90538036-7e43-4b6f-8497-864d66be7d8c",
  "date_created": "2026-02-17T05:53:24.228000Z",
  "date_modified": "2026-02-17T05:53:24.228000Z",
  "file_hash": "4689bf5ec3223686579ee42d478c7023442c5943679b866d8dbed8dab6211f1b",
  "private": false,
  "record": {
    "abstract": "We perform a two-loop calculation in Light Cone Perturbation Theory (LCPT) to evaluate the next-to-leading order nonsinglet splitting function. Our calculation demonstrates the methodology and feasibility of performing higher order calculations in LCPT. Since in Hamiltonian perturbation theory the longitudinal $k^+$ momentum is always positive, poles in $1/k^+$ can be regularized by a simple cutoff which cancels in physical results, without any associated ambiguities. For transverse momentum integrals we use dimensional regularization. Developing methods for loop calculations in LCPT paves the way for a systematical, automatizable procedure for precision calculations in this framework with a transparent physical partonic interpretation. This can provide a standard framework in higher order calculations in the gluon saturation regime of QCD.",
    "arxiv_id": "2601.10374",
    "authors": [
      "Tuomas Lappi",
      "Risto Paatelainen",
      "Mikko Sepp\u00e4l\u00e4"
    ],
    "categories": [
      "hep-ph",
      "nucl-th"
    ],
    "license": "http://creativecommons.org/licenses/by/4.0/",
    "title": "Two-Loop DGLAP Splitting Functions from Light Cone Perturbation Theory",
    "url": "https://arxiv.org/abs/2601.10374",
    "version": "v1"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "dbecc2f7-ba30-4b5f-b901-33316cebde29",
    "id": "arXiv Dataset",
    "type": "Model",
    "variant": "snapshot-2026-01-17",
    "version": "0.1.0"
  },
  "user_id": 1000002
}