{"paper":{"title":"Cartan's Supersymmetry and the Decay of a $h^0$ with the mass $m_{h^0}\\simeq 11$GeV to $\\Upsilon(1S)\\gamma$ and to $\\Upsilon(nS)\\gamma (n=1,2,3)$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Sadataka Furui","submitted_at":"2015-02-25T00:01:56Z","abstract_excerpt":"In the LHCb detector at CERN, decays of $\\chi_b(3P)$ meson to $\\Upsilon(1S)\\gamma$ and $\\Upsilon(2S)\\gamma$ are reported at centre-of-mass energy of $\\sqrt s=7$ and 8 TeV. Following the success of the assignment of $\\chi_b(1P)\\to\\Upsilon(1S)\\gamma$ of the mass of $m(\\chi_b(1P))=9.8923$ GeV and $\\chi_b(2P)\\to\\Upsilon(1S)\\gamma$ of the mass of $m(\\chi_b(2P))=10.2547$ GeV, the new state $\\chi_b(3P)$ of the mass of 10.5157 GeV was assigned, but its $J^{P}$ was not fixed.\n  We study the possibility that this boson is the light Higgs boson $h^0(0^+)$, and study its decay modes to a $b\\bar b$ which r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.07011","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"}