{
  "annotation_id": "fda096c6-1ef1-4dd4-a6e0-c39af7cea4b6",
  "date_created": "2026-03-02T18:00:01.256000Z",
  "date_modified": "2026-03-02T18:00:01.256000Z",
  "file_hash": "0e959b6980be0668a2ccae3332f70fcfddc18cd53dc4faad3c51f4605cf5639b",
  "private": false,
  "record": {
    "abstract": "An operator form of the 3N bound state is proposed. It consists of eight\noperators formed out of scalar products in relative momentum and spin vectors,\nwhich are applied on a pure 3N spin 1/2 state. Each of the operators is\nassociated with a scalar function depending only on the magnitudes of the two\nrelative momenta and the angle between them. The connection between the\nstandard partial wave decomposition of the 3N bound state and the operator form\nis established, and the decomposition of these scalar function in terms of\npartial wave components and analytically known auxiliary functions is given.\nThat newly established operator form of the 3N bound state exhibits the\ndominant angular and spin dependence analytically. The scalar functions are\ntabulated and can be downloaded. As an application the spin dependent nucleon\nmomentum distribution in a polarized 3N bound state is calculated to illustrate\nthe use of the new form of the 3N bound state.",
    "arxiv_id": "nucl-th/0402015",
    "authors": [
      "I. Fachruddin",
      "W. Gloeckle",
      "Ch. Elster",
      "A. Nogga"
    ],
    "categories": [
      "nucl-th",
      "physics.comp-ph"
    ],
    "doi": "10.1103/PhysRevC.69.064002",
    "journal_ref": "Phys.Rev.C69:064002,2004",
    "title": "The Operator form of 3H (3He) and its Spin Structure",
    "url": "https://arxiv.org/abs/nucl-th/0402015"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "305fc166-f3e0-4ed2-a684-f6f12ae50d3f",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}