Semileptonic decays B→D(∗)lνB \to D^{(*)} lν in the perturbative QCD factorization approach

preprint2014arXivOpen access

Abstract

In this paper, we study the B→D(∗)l−νˉlB \to D^{(*)} l^- \barν_{\rm l} semileptonic decays and calculate the branching ratios B(B→D(∗)l−νˉl){\cal B}(B \to D^{(*)} l^- \barν_{\rm l}) and the ratios R(D(∗))R(D^{(*)}) and RDl,τR_{\rm D}^{\rm l,τ} by employing the perturbative QCD (pQCD) factorization approach. We find that (a) for R(D)R(D) and R(D∗)R(D^*) ratios, the pQCD predictions are R(D)=0.430−0.026+0.021R(D)=0.430^{+0.021}_{-0.026}, R(D∗)=0.301±0.013R(D^*)=0.301 \pm 0.013 and agree well with BaBar's measurements of R(D(∗))R(D^{(*)}); (b) for the newly defined RDlR_{\rm D}^{\rm l} and RDτR_{\rm D}^{\rm τ} ratios, the pQCD predictions are RDl=0.450−0.051+0.064R_{\rm D}^{\rm l} = 0.450^{+0.064}_{-0.051} and RDτ=0.642−0.070+0.081R_{\rm D}^{\rm τ} =0.642^{+0.081}_{-0.070}, which may be more sensitive to the QCD dynamics of the considered semileptonic decays than R(D(∗))R(D^{(*)}) and should be tested by experimental measurements.

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