Nonfactorizable decay and QCD factorization
arXiv:hep-ph/0502240 · doi:10.1088/0253-6102/48/5/026
Abstract
We study the unexpectedly large rate for the factorization-forbidden decay within the QCD factorization approach. We use a non-zero gluon mass to regularize the infrared divergences in vertex corrections. The end-point singularities arising from spectator corrections are regularized and carefully estimated by the off-shellness of quarks. We find that the contributions arising from the vertex and leading-twist spectator corrections are numerically small, and the twist-3 spectator contribution with chiral enhancement and linear end-point singularity becomes dominant. With reasonable choices for the parameters, the branching ratio for decay is estimated to be in the range , which is compatible with the Belle and BaBar data.
Appendix added; it is emphasized that in the dominant twist-3 spectator corrections the end-point singularity contributions may be estimated by the off-shellness of the charm quark (by the binding energy in charmonium) and the gluon (by the transverse momentum of the light quark in the kaon)
References in corpus (8)
- The Cosmological Parameters 2006
- Big-Bang nucleosynthesis (Particle Data Group mini-review)
- New Results on B->pi, K, eta Decay Formfactors from Light-Cone Sum Rules
- The B Meson Decay Constant from Unquenched Lattice QCD
- Dalitz analysis of the three-body charmless decays B+=>K+Pi+Pi- and B+=>K+K+K-
- Nonfactorizable contributions to meson decays into charmonia
- decays: a model estimation
- and meson exclusive decay in QCD factorization
Cited by in corpus (8)
- form factors and decays into
- Search for charmonium and bottomonium states in at B factories
- $B \to (\jpsi,η_c) K$ decays in the perturbative QCD approach
- within and beyond the Standard Model
- Branching ratios and asymmetries of decays
- Revisiting nonfactorizable contributions to factorization-forbidden decays of mesons to charmonium
- decays: Results from light-cone QCD Sum Rules
- Resonance contributions from in the charmless three-body hadronic meson decays