Quasi-two-body decays B(s)→Pρ→Pππ in the perturbative QCD approach

Abstract

In this work, we calculate the $CP$-averaged branching ratios and the direct $CP$-violating asymmetries of the quasi-two-body decays $B_{(s)} \to P (\rho \to) \pi\pi$ by employing the perturbative QCD (PQCD) approach (here $P$ stands for a light pseudoscalar meson $\pi, K, \eta$ or $\eta^{\prime}$). The vector current time-like form factor $F_{\pi}$, which contains the final state interactions between the pion pair in the resonant region associated with the $P$-wave states $\rho(770)$ along with the two-pion distribution amplitudes, are employed to describe the interactions between the $\rho$ and the pion pair under the hypothesis of the conserved vector current. We found that (a) the PQCD predictions for the branching ratios and the direct $CP$-violating asymmetries for most considered $B_{(s)} \to P (\rho \to) \pi\pi$ decays agree with currently available data within errors; (b) for ${\cal B}(B \to \pi^0 \rho^0 \to \pi^0(\pi^+ \pi^-)$, the PQCD prediction is much smaller than the measured one; and (c) for $B^+ \to \pi^+(\rho^0\to)\pi^+ \pi^-$ decay mode, we found a negative $CP$ asymmetry $(-27.5^{+3.0}_{-3.7})\%$, which agrees with other theoretical predictions but different in sign from those as reported by BaBar and LHCb Collaboration.