{"paper":{"title":"Superluminal Neutrinos from OPERA Experiment and Weyl Equation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","math.MP"],"primary_cat":"math-ph","authors_text":"E. Capelas de Oliveira, J. Vaz Jr, W. A. Rodrigues Jr.","submitted_at":"2011-10-10T22:21:53Z","abstract_excerpt":"By analyzing the structure of the Weyl spinor field in the Clifford bundle formalism we show that in each spinorial frame it is represented by F\\insec(\\doublebarwedge^0 T^\\starM + \\doublebarwedge^2 T^\\star M + \\doublebarwedge^{4} T^\\star M)\\hookrightarrowsecC\\ell(M,g) satisfying the equation \\partialF=0, where \\partial is the Dirac operator acting on sections of the Clifford bundle C\\ell(M,g). With this result we show that introducing a generalized potential A=(A + \\gamma_5 B)\\insec(\\doublebarwedge^{1}T^{\\star}M + \\doublebarwedge^3 T^\\star M)\\hookrightarrowsecC\\ell(M,g) for the Weyl field such"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.2219","kind":"arxiv","version":1},"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"}