The ρρ-meson longitudinal leading-twist distribution amplitude

preprint2014arXivOpen access

Abstract

In the present paper, we suggest a convenient model for the vector ρρ-meson longitudinal leading-twist distribution amplitude ϕ2;ρ∥ϕ_{2;ρ}^\|, whose distribution is controlled by a single parameter B2;ρ∥B^\|_{2;ρ}. By choosing proper chiral current in the correlator, we obtain new light-cone sum rules (LCSR) for the B→ρB\toρ TFFs A1A_1, A2A_2 and VV, in which the δ1δ^1-order ϕ2;ρ∥ϕ_{2;ρ}^\| provides dominant contributions. Then we make a detailed discussion on the ϕ2;ρ∥ϕ_{2;ρ}^\| properties via those B→ρB\toρ TFFs. A proper choice of B2;ρ∥B^\|_{2;ρ} can make all the TFFs agree with the lattice QCD predictions. A prediction of ∣Vub∣|V_{\rm ub}| has also been presented by using the extrapolated TFFs, which indicates that a larger B2;ρ∥B^{\|}_{2;ρ} leads to a larger ∣Vub∣|V_{\rm ub}|. To compare with the BABAR data on ∣Vub∣|V_{\rm ub}|, the longitudinal leading-twist DA ϕ2;ρ∥ϕ_{2;ρ}^\| prefers a doubly-humped behavior.

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