Extractions of |Vub|/|Vcb| from a combined study of the exclusive $$ b\to u(c){\ell}^{-}{\overline{\nu}}_{\ell } $$ decays

Abstract

Abstract We have extracted the ratio |Vub|/|Vcb| from a combined study of the available inputs on $$ \overline{B}\to \left(\pi, \rho, \omega \right){\ell}^{-}{\overline{\nu}}_{\ell } $$ B ¯ → π ρ ω ℓ − ν ¯ ℓ and $$ \overline{B}\left({\overline{B}}_s\right)\to \left({D}^{\left(\ast \right)},{D}_s^{\left(\ast \right)}\right){\ell}^{-}{\overline{\nu}}_{\ell }\ \left(\ell =\mu\ \textrm{or}\ e\right) $$ B ¯ B ¯ s → D ∗ D s ∗ ℓ − ν ¯ ℓ ℓ = μ or e decays. We have done our analysis with and without the inclusion of the available experimental results on the branching fraction $$ \mathcal{BR}\left({\overline{B}}_s\to {K}^{+}{\mu}^{-}{\overline{\nu}}_{\mu}\right) $$ BR B ¯ s → K + μ − ν ¯ μ or the ratio of the rates $$ \Gamma \left({\overline{B}}_s\to {K}^{+}{\ell}^{-}{\overline{\nu}}_{\ell}\right)/\Gamma \left({\overline{B}}_s\to {D}_s^{+}{\ell}^{-}{\overline{\nu}}_{\ell}\right) $$ Γ B ¯ s → K + ℓ − ν ¯ ℓ / Γ B ¯ s → D s + ℓ − ν ¯ ℓ . We have used all the available experimental data on the branching fractions in different q2-bins, the available theory inputs on the form factors from lattice and the light cone sum rule (LCSR) approach; analysed the data in different possible scenarios and presented the results. From a combined analysis of all the b → cℓ−νℓ exclusive decays, we have obtained |Vcb| = (40.5 ± 0.6) × 10−3 and from all the b → uℓ−νℓ modes, we obtain |Vub| = (3.46 ± 0.12) × 10−3 which changes to |Vub| = (3.51 ± 0.13) × 10−3 after dropping $$ \mathcal{BR}\left({\overline{B}}_s\to {K}^{+}{\mu}^{-}{\overline{\nu}}_{\mu}\right) $$ BR B ¯ s → K + μ − ν ¯ μ . We hence report the values of the ratio |Vub|/|Vcb| = 0.085 ± 0.003 and 0.087 ± 0.003 with and without the input from $$ {\overline{B}}_s\to {K}^{+}{\mu}^{-}{\overline{\nu}}_{\mu } $$ B ¯ s → K + μ − ν ¯ μ modes, respectively. We have also predicted the ratio $$ \Gamma \left({\overline{B}}_s\to {K}^{+}{\ell}^{-}{\overline{\nu}}_{\ell}\right)/\Gamma \left({\overline{B}}_s\to {D}_s^{+}{\ell}^{-}{\overline{\nu}}_{\ell}\right) $$ Γ B ¯ s → K + ℓ − ν ¯ ℓ / Γ B ¯ s → D s + ℓ − ν ¯ ℓ using the fit results. In addition, we provide the predictions of $$ \mathcal{BR}\left({\overline{B}}_s\to {K}^{+}{\mu}^{-}{\overline{\nu}}_{\mu}\right) $$ BR B ¯ s → K + μ − ν ¯ μ and $$ \mathcal{BR}\left(\overline{B}\to \left(\rho, \omega \right){\ell}^{-}{\overline{\nu}}_{\ell}\right) $$ BR B ¯ → ρ ω ℓ − ν ¯ ℓ in the Standard Model (SM) in small q2-bins.