We study the charmless two-body decays of $B\to { \bf B}_n \overline{ \bf B}_n^\prime$ with $B = ( B^+ , B^0 , B^0_s)$ and ${ \bf B}_n^{ (\prime)}$ the low-lying octet baryons. The factorizable amplitudes are calculated by the modified bag model, while the nonfactorizable ones are extracted from the experimental data with the $SU(3)_F$ flavor symmetry. We are able to explain all current experimental measurements and provide predictions on the decay branching ratios in $B\to { \bf B}_n \overline{ \bf B}_n^\prime$. Particularly, we find that ${ \cal B}(B_s^0 \to \Xi^0 \overline{ \Xi}^0) = (19.3\pm 2.7 )\times 10^{ -7}$ and ${ \cal B}(B_s^0 \to \Xi^- \overline{ \Xi}^-) = (19.4\pm 2.7 )\times 10^{ -7}$, which are sizable and able to be observed in the ongoing experiments at LHCb and BELLE-II. Furthermore, the decay branching ratios of $B_s^0 \to (p\overline{ p}, n\overline{ n})$ and $B^0 \to (\Xi^0 \overline{ \Xi}^0 ,\Sigma^+\overline{ \Sigma}^+)$ are expected to be $O(10^{ -10})$, which are suppressed due to the angular momentum conservation and chiral symmetry.
Categories: hep-ph hep-ex