Abstract
In this paper, we make a detailed discussion on the eta and eta ^prime -meson leading-twist light-cone distribution amplitude phi _{2;eta ^{(prime )}}(u,mu ) by using the QCD sum rules approach under the background field theory. Taking both the non-perturbative condensates up to dimension-six and the next-to-leading order (NLO) QCD corrections to the perturbative part, its first three moments langle xi ^n_{2;eta ^{(prime )}}rangle |_{mu _0} with n = (2, 4, 6) can be determined, where the initial scale mu _0 is set as the usual choice of 1 GeV. Numerically, we obtain langle xi _{2;eta }^2rangle |_{mu _0} =0.231_{-0.013}^{+0.010}, langle xi _{2;eta }^4 rangle |_{mu _0} =0.109_{ - 0.007}^{ + 0.007}, and langle xi _{2;eta }^6 rangle |_{mu _0} =0.066_{-0.006}^{+0.006} for eta -meson, langle xi _{2;eta '}^2rangle |_{mu _0} =0.211_{-0.017}^{+0.015}, langle xi _{2;eta '}^4 rangle |_{mu _0} =0.093_{ - 0.009}^{ + 0.009}, and langle xi _{2;eta '}^6 rangle |_{mu _0} =0.054_{-0.008}^{+0.008} for eta '-meson. Next, we calculate the D_srightarrow eta ^{(prime )} transition form factors (TFFs) f^{eta ^{(prime )}}_{+}(q^2) within QCD light-cone sum rules approach up to NLO level. The values at large recoil region are f^{eta }_+(0) = 0.476_{-0.036}^{+0.040} and f^{eta '}_+(0) = 0.544_{-0.042}^{+0.046}. After extrapolating TFFs to the allowable physical regions within the series expansion, we obtain the branching fractions of the semi-leptonic decay, i.e. D_s^+rightarrow eta ^{(prime )}ell ^+ nu _ell , i.e. {{mathcal {B}}}(D_s^+ rightarrow eta ^{(prime )} e^+nu _e)=2.346_{-0.331}^{+0.418}(0.792_{-0.118}^{+0.141})times 10^{-2} and {{mathcal {B}}}(D_s^+ rightarrow eta ^{(prime )} mu ^+nu _mu )=2.320_{-0.327}^{+0.413}(0.773_{-0.115}^{+0.138})times 10^{-2} for ell = (e, mu ) channels respectively. And in addition to that, the mixing angle for eta -eta ' with varphi and ratio for the different decay channels {{mathcal {R}}}_{eta '/eta }^ell are given, which show good agreement with the recent BESIII measurements.
Highlights
The Ds+-meson, which is composed of a charm quark and a strange antiquark, has been discovered in year 1993
In order to show the degree of stability of the transition form factors (TFFs) versus the Borel parameter, we present the curve of TFFs in Fig. 5, in which the shaded region shows the errors from all input parameters
The light-cone sum rules (LCSR) and the covariant confined quark model (CCQM) results are calculated by applying their TFFs into the width formula
Summary
The Ds+-meson, which is composed of a charm quark and a strange antiquark, has been discovered in year 1993. Total semileptonic branching fractions provide useful discrimination on the different theoretical evaluations of hadronic matrix elements, which sizably affect the charm quark semileptonic decays. The η( )-mesons, composed by ssquark pair, are especially intriguing, since the s-quark plays an important role for the flavor physics. The semileptonic decay processes for Ds+ → η( ) +ν have been found by the CLEO collaboration early in year 1995, and their measured value of the ratio of branching fractions B(Ds+ → η e+νe)/B(Ds+ → ηe+νe) is 0.35 ± 0.09 ± 0.07 [7]. The CLEO collaboration issued the measured value of the branching fractions in years 2009
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