Paper detail

$S$, $P$ and $D$-wave resonance contributions to $B_{(s)} \to η_c(1S,2S) Kπ$ decays in the perturbative QCD approach

In this work, we analyze the three-body $B_{(s)} \to η_c(1S,2S) K π$ decays within the framework of the perturbative QCD approach (PQCD) under the quasi-two-body approximation, where the kaon-pion invariant mass spectra are dominated by the $K_0^*(1430)^0,K_0^*(1950)^0,K^*(892)^0,K^*(1410)^0,K^*(1680)^0$ and $K_2^*(1430)^0$ resonances. The time-like form factors are adopted to parametrize the corresponding $S$, $P$, $D$-wave kaon-pion distribution amplitudes for the concerned decay modes, which describe the final-state interactions between the kaon and pion in the resonant region. The $Kπ$ $S$-wave component at low $Kπ$ mass is described by the LASS line shape, while the time-like form factors of other resonances are modeled by the relativistic Breit-Wigner function. We find the following main points: (a) the PQCD predictions of the branching ratios for most considered $B \to η_c(1S)(K^{*0}\to )K^+π^-$ decays agree well with the currently available data within errors; (b) for ${\cal B}(B^0 \to η_c (K_0^*(1430)\to )K^+π^-)$ and ${\cal B}(B^0 \to η_c K^+π^-({\rm NR}))$ (here NR means nonresonant), our predictions of the branching ratios are a bit smaller than the measured ones; and (c) the PQCD results for the $D$-wave contributions considered in this work can be tested once the precise data from the future LHCb and Belle-II experiments are available.