From Ξb→ΛbπΞ_b \to Λ_b π to Ξc→ΛcπΞ_c \to Λ_c π

preprint2016arXivOpen access

Abstract

Using a successful framework for describing S-wave hadronic decays of light hyperons induced by a subprocess s→u(uˉd)s \to u (\bar u d), we presented recently a model-independent calculation of the amplitude and branching ratio for Ξb−→Λbπ−Ξ^-_b \to Λ_b π^- in agreement with a LHCb measurement. The same quark process contributes to Ξc0→Λcπ−Ξ^0_c \to Λ_c π^-, while a second term from the subprocess cs→cdcs \to cd has been related by Voloshin to differences among total decay rates of charmed baryons. We calculate this term and find it to have a magnitude approximately equal to the s→u(uˉd)s \to u (\bar u d) term. We argue for a negligible relative phase between these two contributions, potentially due to final state interactions. However, we do not know whether they interfere destructively or constructively. For constructive interference one predicts B(Ξc0→Λcπ−)=(1.94±0.70)×10−3{\cal B}(Ξ_c^0 \to Λ_c π^-) = (1.94 \pm 0.70)\times 10^{-3} and B(Ξc+→Λcπ0)=(3.86±1.35)×10−3{\cal B}(Ξ_c^+ \to Λ_c π^0) = (3.86 \pm 1.35)\times 10^{-3}. For destructive interference, the respective branching fractions are expected to be less than about 10−410^{-4} and 2×10−42 \times 10^{-4}.

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