Study of Λb→Λ(ϕ,η(′))Λ_b\to Λ(ϕ,η^{(\prime)}) and Λb→ΛK+K−Λ_b\to ΛK^+K^- decays

preprint2016arXivOpen access

Abstract

We study the charmless two-body Λb→Λ(ϕ,η(′))Λ_b\to Λ(ϕ,η^{(\prime)}) and three-body Λb→ΛK+K−Λ_b\to ΛK^+K^- decays. We obtain B(Λb→Λϕ)=(3.53±0.24)×10−6{\cal B}(Λ_b\to Λϕ)=(3.53\pm 0.24)\times 10^{-6} to agree with the recent LHCb measurement. However, we find that B(Λb→Λ(ϕ→)K+K−)=(1.71±0.12)×10−6{\cal B}(Λ_b\to Λ(ϕ\to)K^+ K^-)=(1.71\pm 0.12)\times 10^{-6} is unable to explain the LHCb observation of B(Λb→ΛK+K−)=(15.9±1.2±1.2±2.0)×10−6{\cal B}(Λ_b\toΛK^+ 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 Λb→K−N∗, N∗→ΛK+Λ_b\to K^- N^*,\,N^*\toΛK^+ decay with N∗N^* as a higher-wave baryon state. For Λb→Λη(′)Λ_b\to Λη^{(\prime)}, we show that B(Λb→Λη, Λη′)=(1.47±0.35,1.83±0.58)×10−6{\cal B}(Λ_b\to Λη,\,Λη^\prime)= (1.47\pm 0.35,1.83\pm 0.58)\times 10^{-6}, which are consistent with the current data of (9.3−5.3+7.3,<3.1)×10−6(9.3^{+7.3}_{-5.3},<3.1)\times 10^{-6}, respectively. Our results also support the relation of B(Λb→Λη)≃B(Λb→Λη′){\cal B}(Λ_b\to Λη) \simeq {\cal B}(Λ_b\toΛη^\prime), given by the previous study.

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