{
  "annotation_id": "d74794bb-3a9a-4b2e-9b2b-edcb099e6175",
  "date_created": "2026-03-02T18:00:22.103000Z",
  "date_modified": "2026-03-02T18:00:22.103000Z",
  "file_hash": "21a529d82c4be4d16dbc4d56306fd9647d136d13d62ffc069bdb1ba285026483",
  "private": false,
  "record": {
    "abstract": "The electromagnetic form factors G_E(q^2), G_M(q^2), and G_Q(q^2), charge\nradii, magnetic and quadrupole moments, and decay widths of the light vector\nmesons rho^+, K^{*+} and K^{*0} are calculated in a Lorentz-covariant,\nDyson-Schwinger equation based model using algebraic quark propagators that\nincorporate confinement, asymptotic freedom, and dynamical chiral symmetry\nbreaking, and vector meson Bethe-Salpeter amplitudes closely related to the\npseudoscalar amplitudes obtained from phenomenological studies of pi and K\nmesons. Calculated static properties of vector mesons include the charge radii\nand magnetic moments: r_{rho+} = 0.61 fm, r_{K*+} = 0.54 fm, and r^2_{K*0} =\n-0.048 fm^2; mu_{rho+} = 2.69, mu_{K*+} = 2.37, and mu_{K*0} = -0.40. The\ncalculated static limits of the rho-meson form factors are similar to those\nobtained from light-front quantum mechanical calculations, but begin to differ\nabove q^2 = 1 GeV^2 due to the dynamical evolution of the quark propagators in\nour approach.",
    "arxiv_id": "nucl-th/9806025",
    "authors": [
      "F. T. Hawes",
      "M. A. Pichowsky"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "doi": "10.1103/PhysRevC.59.1743",
    "journal_ref": "Phys.Rev.C59:1743-1750,1999",
    "title": "Electromagnetic form factors of light vector mesons",
    "url": "https://arxiv.org/abs/nucl-th/9806025"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "6ce2390c-8190-4534-a8ca-d557959df11f",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}