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Nonleptonic B decays into a charmed tensor meson

Abstract

In the framework of the factorization and the heavy quark effective theory, Bβ†’D2βˆ—Ο€B\to D_2^*\pi modes are analyzed. We adopt the result from the QCD sum rule calculation for the hadronic matrix elements at leading order of Ξ›QCD/mQ\Lambda_{\rm QCD}/m_Q and Ξ±s\alpha_s. The QCD sum rule results are well compatible with the current data, with the prediction on the branching ratios \calB(\Bbar^0\to D_2^{*+}\pi^-)=8.94\times 10^{-4} and \calB(B^-\to D_2^{*0}\pi^-)=9.53\times 10^{-4} for NCeff=2N_C^{\rm eff}=2. We give constraints on the interception Ο„(1)\tau(1) and the slope parameter ρ2\rho^2 of the leading Isgur-Wise function from the experimental bounds. It is argued that the observation of nonzero \calB(\Bbar^0\to D_2^{*0}\pi^0) directly measures the nonfactorizable effets.Comment: More discussions, references added, to appear in Eur. Phys. J.

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