A bstract We investigate the inverse moment of the B s -meson light-cone distribution amplitude (LCDA), denoted as λBₛ λ B s and defined within the heavy quark effective theory, through the calculation of B s → η s form factors. The presence of the s -quark inside the B s -meson dictates a notable departure of approximately 20% in the λBₛ λ B s value compared to the non-strange case λBq λ B q , as computed within the QCD sum rule approach, albeit with significant uncertainty. First, we compute the decay constant of the η s -meson utilizing two-point sum rules while retaining finite s -quark mass contributions. Next, we constrain the parameter λBₛ λ B s by calculating B s → η s form factors within the light-cone sum rule approach, using B s -meson LCDAs, and leveraging Lattice QCD estimates at zero momentum transfer from the HPQCD collaboration. Our findings yield λBₛ λ B s = 480 ± 92 MeV when expressing the B s -meson LCDAs in the Exponential model, consistent with previous QCD sum rule estimate yet exhibiting a 1.5-fold improvement in uncertainty. Furthermore, we compare the form factor predictions, based on the extracted λBₛ λ B s value, with earlier analyses for other channels such as B s → D s and B s → K .
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Mandal et al. (2024) studied this question.
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