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Contribution of bsggb \to sgg through the QCD anomaly in exclusive decays B±(η,η)(K±,K±)B^{\pm}\to (\eta^{\prime},\eta)(K^{\pm}, K^{*\pm}) and B0(η,η)(K0,K0)B^{0}\to (\eta^{\prime},\eta)(K^{0},K^{*0})

Abstract

We compute the decay rates for the exclusive decays B±(η,η)(K±,K±)B^{\pm} \to (\eta^{\prime},\eta) (K^{\pm}, K^{*\pm}) and B0(η,η)(K0,K0)B^{0}\to (\eta^{\prime},\eta) (K^{0}, K^{*0}) in a QCD-improved factorization framework by including the contribution from the process bsggs(η,η)b\to sgg \to s (\eta^{\prime}, \eta) through the QCD anomaly. This method provides an alternative estimate of the contribution bsccˉs(η,η)b \to s c\bar{c} \to s(\eta,\eta^\prime) to these decays as compared to the one using the intrinsic charm content of the η\eta^{\prime} and η\eta mesons determined through the decays J/ψ(η,η,ηc)γJ/\psi \to (\eta,\eta^\prime ,\eta_c) \gamma. The resulting branching ratios are compared with the CLEO data on B±ηK±B^{\pm} \to \eta^{\prime} K^{\pm} and B0ηK0B^{0} \to \eta^{\prime} K^{0} and predictions are made for the rest.Comment: 16 pages including 4 postscript figures; uses epsfig. The most recent branching ratios from CLEO, ref. [5], are taken into account. The theory part is unchange

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