{"paper":{"title":"Cartan's Supersymmetry and Weak and Electromagnetic Interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Sadataka Furui","submitted_at":"2015-02-16T13:20:30Z","abstract_excerpt":"We apply the Cartan's supersymmetric model to the weak interaction of hadrons. The electromagnetic currents are transformed by $G_{12},G_{123},G_{13},G_{132}$ and the factor$(1-\\gamma_5)$ is inserted between $l \\bar\\nu$ or $\\bar l \\nu$ when the photon is replaced by $W^\\pm$, and between $l \\bar l$ or $\\nu\\bar \\nu$ when the photon is replaced by $Z$.\n  Electromagnetic currents in the Higgs boson $H^0$ decay into 2$\\gamma$ and $D_s(0^+)$ decay into $D_s(0^-)\\pi$ and $D_s(0^-)\\gamma$ in which leptons are replaced by quarks are also studied.\n  A possibility that the boson near the $B\\bar B$ thesho"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.04524","kind":"arxiv","version":4},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}