In this paper, moments of $a_0(980)$-meson twist-2 light-cone distribution amplitudes were deeply researched by using QCD sum rules approach within background field theory. Up to 9th-order accuracy, we present $\langle\xi_{ 2;a_0}^n\rangle|_{ \mu_0}$ at the initial scale $\mu_0 = 1~{ \rm GeV}$, i.e. $\langle\xi^1_{ 2;a_0}\rangle|_{ \mu_0} = -0.307(43)$, $\langle\xi^3_{ 2;a_0}\rangle|_{ \mu_0} = -0.181(34)$, $\langle\xi^5_{ 2;a_0}\rangle|_{ \mu_0} = -0.078(28)$, $\langle\xi^7_{ 2;a_0}\rangle|_{ \mu_0} = -0.049(26)$, $\langle\xi^9_{ 2;a_0}\rangle|_{ \mu_0} = -0.036(24)$, respectively. An improved light-cone harmonic oscillator model for $a_0(980)$-meson twist-2 light-cone distribution amplitudes is adopted, where its parameters are fixed by using the least squares method based on the $\langle\xi_{ 2;a_0}^n\rangle|_{ \mu_0}$, and their goodness of fit reach to $95.4\%$. Then, we calculate the $D\to a_0(980)$ transition form factors within the light-cone sum rules approach, and at largest recoil point, we obtain $f_+^{ D\to a_0}(0) = 1.058^{ +0.068}_{ -0.035}$ and $f_-^{ D\to a_0}(0) = 0.764^{ +0.044}_{ -0.036}$. As a further application, the branching fractions of the $D\to a_0(980)\ell\bar\nu_\ell$ semileptonic decays are given. Taking the decay $a_0(980)\to \eta\pi$ into consideration, we obtain ${ \cal B}(D^0 \to a_0(980)^- (\to \eta \pi^-) e^+\nu_e) =(1.330^{ +0.216}_{ -0.134})\times10^{ -4}$, ${ \cal B}(D^+\to a_0(980)^0(\to \eta \pi^0)e^+\nu_e)=(1.675^{ +0.272}_{ -0.169})\times10^{ -4}$, which are consistent with the BESIII collaboration and PDG data within errors. Finally, we present the angle observables of forward-backward asymmetries, $q^2$-differential flat terms and lepton polarization asymmetry of the semileptonic decay $D\to a_0(980)\ell\bar\nu_\ell$.
Categories: hep-ph