{
  "annotation_id": "d687c4d2-2b6f-43cb-b3a0-f27cb5c99e43",
  "date_created": "2026-03-02T18:00:01.536000Z",
  "date_modified": "2026-03-02T18:00:01.536000Z",
  "file_hash": "e7c697055737fddc3a34762f7c9610fff5dee71915b6e9afcfc6f8a5d908921a",
  "private": false,
  "record": {
    "abstract": "We discuss a sum rule satisfied by the correlation function of two particles\nwith small relative momenta. The sum rule, which results from the completeness\ncondition of the quantum states of the two particles, is first derived and then\nwe check how it works in practice. The sum rule is shown to be trivially\nsatisfied by free particle pair, and then there are considered three different\nsystems of interacting particles. We discuss a pair of neutron and proton in\nthe s-wave approximation and the case of the so-called hard spheres with the\nphase shifts taken into account up to l=4. Finally, the Coulomb system of two\ncharged particles is analyzed.",
    "arxiv_id": "nucl-th/0409061",
    "authors": [
      "Radoslaw Maj",
      "Stanislaw Mrowczynski"
    ],
    "categories": [
      "nucl-th",
      "hep-ph",
      "nucl-ex"
    ],
    "doi": "10.1103/PhysRevC.71.044905",
    "journal_ref": "Phys.Rev. C71 (2005) 044905",
    "title": "Sum rule of the correlation function",
    "url": "https://arxiv.org/abs/nucl-th/0409061"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "cf191a12-a5ed-4f30-a3bf-4270eac93281",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}