Study of charmless two-body baryonic BB decays

preprint2022arXivOpen access

Abstract

We study the charmless two-body decays of B→BnB‾n′B\to {\bf B}_n \overline{\bf B}_n^\prime with B=(B+,B0,Bs0)B = ( B^+ , B^0 , B^0_s) and Bn(′){\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)FSU(3)_F flavor symmetry. We are able to explain all current experimental measurements and provide predictions on the decay branching ratios in B→BnB‾n′B\to {\bf B}_n \overline{\bf B}_n^\prime. Particularly, we find that B(Bs0→Ξ0Ξ‾0)=(19.3±2.7)×10−7{\cal B}(B_s^0 \to Ξ^0 \overlineΞ^0) = (19.3\pm 2.7 )\times 10^{-7} and B(Bs0→Ξ−Ξ‾−)=(19.4±2.7)×10−7{\cal B}(B_s^0 \to Ξ^- \overlineΞ^-) = (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 Bs0→(pp‾,nn‾)B_s^0 \to (p\overline{p}, n\overline{n}) and B0→(Ξ0Ξ‾0,Σ+Σ‾+)B^0 \to (Ξ^0 \overlineΞ^0 ,Σ^+\overlineΣ^+) are expected to be O(10−10)O(10^{-10}), which are suppressed due to the angular momentum conservation and chiral symmetry.

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