{"paper":{"title":"Exploring the $\\Upsilon(6S)\\to \\chi_{bJ}\\phi$ and $\\Upsilon(6S)\\to \\chi_{bJ}\\omega$ hidden-bottom hadronic transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Bo Wang, Dian-Yong Chen, Qi Huang, Takayuki Matsuki, Xiang Liu","submitted_at":"2017-01-04T04:03:22Z","abstract_excerpt":"In this work, we investigate the hadronic loop contributions to the $\\Upsilon(6S) \\to \\chi_{bJ} \\phi~(J=0,1,2)$ along with $\\Upsilon(6S) \\to \\chi_{bJ} \\omega~(J=0,1,2)$ transitions. We predict that the branching ratios of $\\Upsilon(6S) \\to \\chi_{b0} \\phi$, $\\Upsilon(6S) \\to \\chi_{b1} \\phi$ and $\\Upsilon(6S) \\to \\chi_{b2} \\phi$ are $(0.68 \\sim 4.62) \\times 10^{-6}$, $(0.50 \\sim 3.43) \\times 10^{-6}$ and $(2.22 \\sim 15.18) \\times 10^{-6}$, respectively and those of $\\Upsilon(6S) \\to \\chi_{b0} \\omega$, $\\Upsilon(6S) \\to \\chi_{b1} \\omega$ and $\\Upsilon(6S) \\to \\chi_{b2} \\omega$ are $(0.15 \\sim 2.8"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.00894","kind":"arxiv","version":2},"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"}