Study of the quasi-two-body decays B^{0}_{s} \rightarrow ψ(3770)(ψ(3686))π^+π^- with perturbative QCD approach

Abstract

In this note, we study the contributions from the S-wave resonances, f_{0}(980) and f_{0}(1500), to the B^{0}_{s}\rightarrow ψ(3770)π^ {+}π^{-} decay by introducing the S-wave ππdistribution amplitudes within the framework of the perturbative QCD approach. Both resonant and nonresonant contributions are contained in the scalar form factor in the S-wave distribution amplitude Φ^S_{ππ}. Since the vector charmonium meson ψ(3770) is a S-D wave mixed state, we calculated the branching ratios of S-wave and D-wave respectively, and the results indicate that f_{0}(980) is the main contribution of the considered decay, and the branching ratio of the ψ(2S) mode is in good agreement with the experimental data. We also take the S-D mixed effect into the B^{0}_{s}\rightarrow ψ(3686)π^ {+}π^{-} decay. Our calculations show that the branching ratio of B^{0}_{s}\rightarrow ψ(3770)(ψ(3686))π^ {+}π^{-} can be at the order of 10^{-5}, which can be tested by the running LHC-b experiments.

arXiv comment10 pages, 3 figures

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Cited by in corpus (3)

• Two-Meson Form Factors in Unitarized Chiral Perturbation Theory
• Study of the four-body decays $B_S^0\to \pi \pi \pi \pi$ in the perturbative QCD approach
• Investigating $B_s$ three-body decays to scalar mesons in perturbative QCD approach