{
  "annotation_id": "eb3d6228-3409-4a99-b9b7-be3a73621d8a",
  "date_created": "2026-03-02T18:00:11.966000Z",
  "date_modified": "2026-03-02T18:00:11.966000Z",
  "file_hash": "226a9cca9198710fda0a4ff0bda144e74e2bba15897624689f95601b451f5280",
  "private": false,
  "record": {
    "abstract": "A purely left-chiral model of the weak interactions is used to show that the\ntotal parity-violating asymmetry in quark-quark scattering must grow with\nincreasing energy. In the absence of other new physics, non-observation of a\nlarge asymmetry can therefore be used to infer an upper bound on the mass scale\nfor new right-chiral weak vector bosons. Applying this idea to actual\nnucleon-nucleon scattering requires more involved calculations, as the dominant\ncontribution appears to come from a component of diquark-quark scattering\nrelated to, but not identical to, wavefunction-mixing. Earlier criticism of\nthis model by Simonius and Unger is refuted and a new calculation is proposed\nas an additional check on the result. Finally, we argue that the so-called\n`spin crisis\u0027 does not affect our conclusions. (Talk given at the BNL workshop\non future directions in particle and nuclear physics at multi-GeV hadron beam\nfacilities, March 4--6, 1993.)",
    "arxiv_id": "nucl-th/9304020",
    "authors": [
      "T. Goldman"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "title": "No-Lose `Theorem\u0027 for Parity Violating Nucleon-Nucleon Scattering   Experiments",
    "url": "https://arxiv.org/abs/nucl-th/9304020"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "6788ca64-b476-498a-b290-eb8947c578f4",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}