{"paper":{"title":"Study of $\\Lambda_b\\to \\Lambda (\\phi,\\eta^{(\\prime)})$ and $\\Lambda_b\\to \\Lambda K^+K^-$ decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"C.Q. Geng, Yao Yu, Y.K. Hsiao, Yu-Heng Lin","submitted_at":"2016-03-22T06:43:58Z","abstract_excerpt":"We study the charmless two-body $\\Lambda_b\\to \\Lambda (\\phi,\\eta^{(\\prime)})$ and three-body $\\Lambda_b\\to \\Lambda K^+K^- $ decays. We obtain ${\\cal B}(\\Lambda_b\\to \\Lambda\\phi)=(3.53\\pm 0.24)\\times 10^{-6}$ to agree with the recent LHCb measurement. However, we find that ${\\cal B}(\\Lambda_b\\to \\Lambda(\\phi\\to)K^+ K^-)=(1.71\\pm 0.12)\\times 10^{-6}$ is unable to explain the LHCb observation of ${\\cal B}(\\Lambda_b\\to\\Lambda K^+ K^-)=(15.9\\pm 1.2\\pm 1.2\\pm 2.0)\\times 10^{-6}$, which implies the possibility for other contributions, such as that from the resonant $\\Lambda_b\\to K^- N^*,\\,N^*\\to\\Lamb"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.06682","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"}