Abstract

More than two decades ago, we studied heavy-flavor-conserving weak decays of heavy baryons within the framework that incorporates both heavy-quark and chiral symmetries. In view of the first observation of Ξb−→Λb0π−Ξ_b^-\toΛ_b^0π^- by LHCb recently, we have reexamined these decays and presented updated predictions. The predicted rates for Ξb−→Λb0π−Ξ_b^-\toΛ_b^0π^- in the MIT bag and diquark models are consistent with experiment. The major theoretical uncertainty stems from the evaluation of baryon matrix elements. The branching fraction of Ξc→ΛcπΞ_c\toΛ_cπ is predicted to be of order 10−410^{-4}. It is suppressed relative to Br(Ξb→Λbπ)Br(Ξ_b\toΛ_bπ) owing to the shorter lifetime of ΞcΞ_c relative to ΞbΞ_b and the destructive nonspectator WW-exchange contribution. The kinematically accessible weak decays of the sextet heavy baryon ΩQΩ_Q are ΩQ→ΞQπΩ_Q\toΞ_Qπ. Due to the absence of the B6−B3ˉB_6-B_{\bar 3} transition in the heavy quark limit and the B6−B6B_6-B_6 transition in the model calculations, ΩQ→ΞQπΩ_Q\toΞ_Qπ vanish in the heavy quark limit.

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