{
  "annotation_id": "78eb4db2-c2d7-4943-adee-59899421b44d",
  "date_created": "2026-03-02T18:00:22.451000Z",
  "date_modified": "2026-03-02T18:00:22.451000Z",
  "file_hash": "ef74eff648bf45edf680905cce3d75fd11cb5675fc8fc1062ef0514392a57ece",
  "private": false,
  "record": {
    "abstract": "Relativistic integral representation in terms of experimental neutron-proton\nscattering phase shifts alone is used to compute the charge form factor of the\ndeuteron $G_{Cd}(Q^2)$. The results of numerical calculations of\n$|G_{Cd}(Q^2)|$ are presented in the interval of the four-momentum transfers\nsquared $0 \\leq Q^2 \\leq 35 fm^{-2}$. Zero and the prominent secondary maximum\nin $ |G_{Cd}(Q^2)|$ are the direct consequences of the change of sign in the\nexperimental $^3S_1$- phase shifts. Till the point $Q^2 \\simeq 20 fm^{-2}$ the\ntotal relativistic correction to $|G_{Cd}(Q^2)|$ is positive and reaches the\nmaximal value of 25% at $Q^2 \\simeq 14 fm^{-2}$.",
    "arxiv_id": "nucl-th/9712082",
    "authors": [
      "Andrei V. Afanasev",
      "V. D. Afanasev",
      "S. V. Trubnikov"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "title": "Relativistic Charge Form Factor of the Deuteron",
    "url": "https://arxiv.org/abs/nucl-th/9712082"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "07f1f05e-9241-475f-889e-78305ca99241",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}