Abstract
Inspired by the recent measurement of the ratio of $B_c$ branching fractions to $J/\psi \pi^+$ and $J/\psi \mu^+\nu_{\mu}$ final states at the LHCb detector, we study the semileptonic decays of $B_c$ meson to the S-wave ground and radially excited 2S and 3S charmonium states with the perturbative QCD approach. After evaluating the form factors for the transitions $B_c\rightarrow P,V$, where $P$ and $V$ denote pseudoscalar and vector S-wave charmonia, respectively, we calculate the branching ratios for all these semileptonic decays. The theoretical uncertainty of hadronic input parameters are reduced by utilizing the light-cone wave function for $B_c$ meson. It is found that the predicted branching ratios range from $10^{-6}$ up to $10^{-2}$ and could be measured by the future LHCb experiment. Our prediction for the ratio of branching fractions $\frac{\mathcal {BR}(B_c^+\rightarrow J/\Psi \pi^+)}{\mathcal {BR}(B_c^+\rightarrow J/\Psi \mu^+\nu_{\mu})}$ is in good agreement with the data. For $B_c\rightarrow V l \nu_l$ decays, the relative contributions of the longitudinal and transverse polarization are discussed in different momentum transfer squared regions. These predictions will be tested on the ongoing and forthcoming experiments.
Highlights
The LHCb Collaboration has measured the semileptonic and hadronic decay rates of the Bc meson and obtainedBR( Bc+ → J / BR( Bc+ → J / π+) μ+ νμ ) =0.0469 ± 0.0028(stat) ± 0.0046(syst)There are many theoretical approaches to the calculation of Bc meson semileptonic decays to charmonium
In our previous work [27,28], we analyzed the two-body nonleptonic decays of the Bc meson with the final states involving one S-wave charmonium using the perturbative QCD based on kT factorization
By using the harmonicosillator wave functions for the charmonium states, the obtained ratios of the branching fractions are consistent with the data and other studies
Summary
The LHCb Collaboration has measured the semileptonic and hadronic decay rates of the Bc meson and obtained. There are many theoretical approaches to the calculation of Bc meson semileptonic decays to charmonium. In our previous work [27,28], we analyzed the two-body nonleptonic decays of the Bc meson with the final states involving one S-wave charmonium using the perturbative QCD based on kT factorization. The semileptonic decays Bc → (J/ψ, ηc)lν have been studied in pQCD [31], compared to which the new ingredients of this paper are the following. Its invariant mass vanishes, while the charm quark in the final states is proportional to the charmonium meson momentum and its invariant mass does not vanish. This substantial revision will render our analysis more consistent. The evaluation of the 3S charmonium distribution amplitudes is relegated to the appendix
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