The B→D(∗)lνlB\to D^{(*)} lν_l decays in the pQCD approach with the Lattice QCD input

preprint2015arXivOpen access

Abstract

In this paper, we studied the semileptonic decays B→D(∗)l−νˉlB \to D^{(*)} l^- \barν_l by using the "pQCD+Lattice QCD" method. We made the extrapolation for the six relevant form factors by using the input values obtained from the pQCD factorization approach in the low q2q^2 region of 0≤q2≤mτ20\leq q^2 \leq m_τ^2, and the Lattice QCD input at the end-point q2=qmax2q^2=q^2_{\rm max}. We then calculated the ratios R(D)R(D) and R(D∗)R(D^*) of the branching ratios B(B→D(∗)l−νˉl){\cal B}(B \to D^{(*)} l^- \barν_l), and found numerically that (1) the "pQCD+Lattice QCD" predictions for the branching ratios B(B→D(∗)l−νˉl){\cal B}(B \to D^{(*)} l^-\barν_l) agree well with the measured values within one standard deviation, and (2) the "pQCD+Lattice QCD" predictions for the ratios R(D(∗))R(D^{(*)}) are R(D)=0.337−0.037+0.038 R(D)=0.337^{+0.038}_{-0.037} and R(D∗)=0.269−0.020+0.021 R(D^*)=0.269^{+0.021}_{-0.020}, they agree with the data within 2σ2σ deviation, in other words, one can explain the "R(D(∗))R(D^{(*)})-puzzle" in the framework of the standard model.

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