Charmless B -> VV Decays in QCD Factorization: Implications of Recent Measurement
arXiv:hep-ph/0104090 · doi:10.1016/S0370-2693(01)00606-2
Abstract
In the heavy quark limit, both vector mesons in the charmless B -> VV decay should have zero helicity and the corresponding amplitude is proportional to the form factor difference . The first observed charmless mode, , indicates that the form factors and cannot be very similar at low as shown in some form-factor models. The approach of QCD-improved factorization implies that the nonfactorizable correction to each partial-wave or helicity amplitude is not the same; the effective parameters vary for different helicity amplitudes. The leading-twist nonfactorizable corrections to the transversely polarized amplitudes vanish in the chiral limit and hence it is necessary to take into account twist-3 distribution amplitudes of the vector meson in order to have renormalization scale and scheme independent predictions. Branching ratios of decays are calculated in two different models for form factors, and the predicted decay rates are different by a factor of . Owing to the absence of (S-P)(S+P) penguin contributions to the W-emission amplitudes, tree-dominated decays tend to have larger branching ratios than the penguin-dominated ones.
11 pages. A sign typo in Eq.(14) is corrected. Experimental data are updated. To appear in PLB
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