The , decays in the perturbative QCD approach
arXiv:1505.02498 · doi:10.1140/epjc/s10052-015-3528-0
Abstract
Nonleptonic two body decays including radially excited or mesons in the final state are studied using the perturbative QCD approach based on factorization. The charmonium distribution amplitudes are extracted from the Schrdinger states for the harmonic oscillator potential. Utilizing these distribution amplitudes, we calculate the numerical results of the transition form factors and branching fractions of decays. The ratio between two decay modes and is compatible with the experimental data within uncertainties, which indicate that the harmonic oscillator wave functions for and work well. It is found that the branching fraction of , which is dominated by the twist-3 charmonium distribution amplitude, can reach the order of . We hope it can be measured soon in the LHCb experiment.
9 pages, 3 figures,3 Tables
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Cited by in corpus (7)
- The S-wave resonance contributions in the decays into plus pion pair
- Relativistic corrections to light-cone distribution amplitudes of S-wave mesons and heavy quarkonia
- Quasi-two-body decays in the perturbative QCD approach
- Quasi-two-body decays in the perturbative QCD approach
- Exclusive nonleptonic Bc-meson decays to S-wave charmonium states
- Branching ratios, asymmetries and polarizations of decays
- Charmless decays in the QCD factorization approach