Two-body Baryonic Bu,d,sB_{u,d,s} and BcB_c to Charmless Final State Decays

preprint2022arXivOpen access

Abstract

We study the rates and direct CP violations of two-body baryonic Bˉu,d,s→BB‾′\bar B_{u,d,s}\to {{\rm\bf B}\overline{\rm\bf B}}' and Bc−→BB‾′B^-_c\to{{\rm\bf B}\overline{\rm\bf B}}' decays, where the final state baryons include low-lying octet and decuplet baryons. We incorporate topological amplitude formalism and the factorization approach. Asymptotic relations at large mbm_b are used to simplify decay amplitudes. Using the most up-to-date data on Bˉ0→ppˉ\bar B^0\to p\bar p and B−→ΛpˉB^-\toΛ\bar p decay rates as inputs, rates and direct CP violations of Bˉu,d,s→BB‾′\bar B_{u,d,s}\to {{\rm\bf B}\overline{\rm\bf B}}' decays are revised and predicted. It is interesting that the results on rates satisfy all existing experimental bounds and some are close to the bounds. Factorization diagrams contribute to penguin-exchange, exchange, annihilation and penguin-annihilation amplitudes. Although the resulting penguin-exchange factorization amplitudes are sizable, the rest suffer from severe chiral suppression and are sensitive to non-factorizable contributions. The Bˉs→ppˉ\bar B_s\to p\bar p decay rate predicted in factorization calculation is very rare, but it can be enhanced by including non-factorizable contributions. The case where the rate is enhanced to saturate the present experimental bound is discussed. As annihilation modes Bc−→BB‾′B^-_c\to{{\rm\bf B}\overline{\rm\bf B}}' decays from factorization calculation are found to be very rare, but they can be enhanced by including non-factorizable contributions as well. Small direct CP violations of pure penguin modes in ΔS=−1ΔS=-1 Bˉu,d,s→BB‾′\bar B_{u,d,s}\to{{\rm\bf B}\overline{\rm\bf B}}' decays are robust predictions of the SM, while vanishing direct CP violations of exchange modes in Bˉu,d,s→BB‾′\bar B_{u,d,s}\to{{\rm\bf B}\overline{\rm\bf B}}' decays and in all Bc−→BB‾′B^-_c\to{{\rm\bf B}\overline{\rm\bf B}}' decay modes are null tests of the SM.

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