S-wave nonleptonic hyperon decays and ${\mathrm{\Xi }}_b^{-}\to {\pi }^{-}{\mathrm{\Lambda }}_b$

The decay ${\mathrm{\Xi }}_b^{-}\to {\pi }^{-}{\mathrm{\Lambda }}_b$ has recently been observed by the LHCb Collaboration at CERN. In contrast to most weak decays of $b$-flavored baryons, this process involves the decay of the strange quark in ${\mathrm{\Xi }}_b$, and thus has features in common with nonleptonic weak decays of hyperons. Thanks to the expected pure S-wave nature of the decay in question in the heavy $b$ quark limit, we find that its amplitude may be related to those for S-wave nonleptonic decays of $\mathrm{\Lambda }$, $\mathrm{\Sigma }$, and $\mathrm{\Xi }$ in a picture inspired by duality. The calculated branching fraction ${\cal B}(\Xi^-_b \to \pi^- \Lambda_b) = (6.3 \pm 4.2) \times 10^{-3}$ is consistent with the range allowed in the LHCb analysis. The error is dominated by an assumed 30% uncertainty in the amplitude due to possible U(3) violation. A more optimistic view based on sum rules involving nonleptonic hyperon decay S-wave amplitudes reduces the error on the branching fraction to $2.0\times {10}^{-3}$.