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

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

2007-02-22

arxiv.org/abs/hep-ph/0702229v2

Physics

High Energy Physics

High Energy Physics - Phenomenology

6 pages, no figures; revtex4

Scientific paper

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 $\eta_D =f_{D_s}/f_D\approx 1.23(15)$, recently observed in the CLEO experiment, and $\eta_B=f_{B_s}/f_B\approx 1.20$, 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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