Extraction of a1a_1 and a2a_2 from B→ψK(K∗), D(D∗)π(ρ)B\to ψK(K^*),~ D(D^*)π(ρ) Decays

preprint1994arXivOpen access

Abstract

Based on the factorization approach, we show that the CLEO data for the ratio Γ(B→ψK∗)/Γ(B→ψK)Γ(B\toψK^*)/Γ(B\to ψK) and the CDF measurement of the fraction of longitudinal polarization in B→ψK∗B\toψK^* can be accounted for by the heavy-flavor-symmetry approach for heavy-light form factors provided that the form factor F0F_0 behaves as a constant, while the q2q^2 dependence is of the monopole form for F1, A0, A1F_1,~ A_0,~A_1, and of the dipole behavior for A2A_2 and VV. This q2q^2 extrapolation for form factors is further supported by B→K∗γB\to K^*γ data and by a recent QCD-sum-rule analysis. We then apply this method to B→D(D∗)π(ρ)B\to D(D^*)π(ρ) decays to extract the parameters a1a_1 and a2a_2. It is found that a1(B→D(∗)π(ρ))=1.01±0.06a_1(B\to D^{(*)}π(ρ))=1.01\pm 0.06 and a2(B→D(∗)π(ρ))=0.23±0.06 a_2(B\to D^{(*)}π(ρ))=0.23\pm 0.06\,. Our result a2/a1=0.22±0.06a_2/a_1=0.22\pm 0.06 thus significantly improves the previous analysis that leads to a2/a1=0.23±0.11a_2/a_1=0.23\pm 0.11. We argue that, contrary to what anticipated from the leading 1/Nc1/N_c expansion, the sign of $a_2(B\toψ\K)$ should be positive and $a_2(B\toψ\K)~{\large ^>_\sim}~ a_2(B\to D^{(*)}π(ρ))$.

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