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arXiv · hep-ph/0702229

The running mass $m_s$ at low scalefrom the heavy-light meson decay constants

A. M. Badalian·B. L. G. Bakker
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Abstract

It is shown that a 25(20)% difference between the decay constants $f_{D_s}(f_{B_s})$ and $f_D(f_B)$ occurs due to large differences in the pole masses of the $s$ and $d(u)$ quarks. The values $η_D =f_{D_s}/f_D\approx 1.23(15)$, recently observed in the CLEO experiment, and $η_B=f_{B_s}/f_B\approx 1.20$, obtained in unquenched lattice QCD, can be reached only if the running mass $m_s$ at low scale is $m_s(\sim 0.5 $ GeV)$= 170 - 200$ MeV. Our results follow from the analytical expression for the pseudoscalar decay constant $f_{\rm P}$ based on the path-integral representation of the meson Green's function.

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A. M. Badalian, B. L. G. Bakker. 2008-03-12. The running mass $m_s$ at low scalefrom the heavy-light meson decay constants. https://doi.org/10.1134/s0021364007220043

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