The $D_s$-meson leading-twist distribution amplitude within the QCD sum rules and its application to the $B_s\to D_s$ transition form factor

Abstract

We make a detailed study on the $D_s$ meson leading-twist LCDA ${\varphi }_{2;D_s}$ by using the QCD sum rules within the framework of the background field theory. To improve the precision, its moments $⟨{\xi }^n{⟩}_{2;D_s}$ are calculated up to dimension-six condensates. At the scale $\mu =2\mathrm{GeV}$, we obtain: $⟨{\xi }^1{⟩}_{2;D_s}=-0.261_{-0.020}^{+0.020}$, $⟨{\xi }^2{⟩}_{2;D_s}=0.184_{-0.012}^{+0.012}$, $⟨{\xi }^3{⟩}_{2;D_s}=-0.111_{-0.012}^{+0.007}$ and $⟨{\xi }^4{⟩}_{2;D_s}=0.075_{-0.005}^{+0.005}$. Using those moments, the ${\varphi }_{2;D_s}$ is then constructed by using the light-cone harmonic oscillator model. As an application, we calculate the transition form factor $f_{+}^{B_s\to D_s}(q^2)$ within the light-cone sum rules (LCSR) approach by using a right-handed chiral current, in which the terms involving ${\varphi }_{2;D_s}$ dominates the LCSR. It is noted that the extrapolated $f_{+}^{B_s\to D_s}(q^2)$ agrees with the Lattice QCD prediction. After extrapolating the transition form factor to the physically allowable $q^2$-region, we calculate the branching ratio and the CKM matrix element, which give $\mathcal{B}({\bar{B}}_s^0\to D_s^{+}\ell {\nu }_{\ell })=(2.03_{-0.49}^{+0.35})\times 10^{-2}$ and $|V_{cb}|=(40.00_{-4.08}^{+4.93})\times 10^{-3}$.

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Cited by in corpus (12)

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• Form factors and branching fraction calculations for $B_s\to D_s^{(\ast )}{\ell }^{+}{\nu }_{\ell }$ in view of LHCb observation
• $K_0^{\ast }(1430)$ Twist-2 Distribution Amplitude and $B_s,D_s\to K_0^{\ast }(1430)$ Transition Form Factors
• $a_0(980)$-meson twist-2 distribution amplitude within the QCD sum rules and investigation of $D\to a_0(980)(\to \eta \pi )e^{+}{\nu }_e$
• $a_1(1260)$-meson longitudinal twist-2 distribution amplitude and the $D\to a_1(1260){\ell }^{+}{\nu }_{\ell }$ decay processes
• The ratio $\mathcal{R}(D_s)$ for $B_s\to D_s\ell {\nu }_{\ell }$ by using the QCD light-cone sum rules within the framework of heavy quark effective field theory
• Systematic analysis of the form factors of $B_c$ to $P$-wave charmonia and corresponding weak decays
• Longitudinal leading-twist distribution amplitude of the ${}^1{P}_1$-state $b_1(1235)$ meson and its implications on $B\to b_1(1235){\ell }^{+}{\nu }_{\ell }$ decays
• Searching for $a_0(980)$-meson parton distribution function
• Probing $D_s^{\ast }$-meson longitudinal twist-2 LCDA
• ${\eta }_c$ leading-twist distribution amplitude and the $B_c\to {\eta }_c\ell {\bar{\nu }}_{\ell }$ semileptonic decays using QCD Sum Rules
• ${\eta }^{(\prime )}$-meson twist-2 distribution amplitude within QCD sum rule approach and its application to the semi-leptonic decay $D_s^{+}\to {\eta }^{(\prime )}{\ell }^{+}{\nu }_{\ell }$