English

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

High Energy Physics - Phenomenology 2015-06-25 v2 High Energy Physics - Experiment

Abstract

It is shown that a 25(20)% difference between the decay constants fDs(fBs)f_{D_s}(f_{B_s}) and fD(fB)f_D(f_B) occurs due to large differences in the pole masses of the ss and d(u)d(u) quarks. The values ηD=fDs/fD1.23(15)\eta_D =f_{D_s}/f_D\approx 1.23(15), recently observed in the CLEO experiment, and ηB=fBs/fB1.20\eta_B=f_{B_s}/f_B\approx 1.20, obtained in unquenched lattice QCD, can be reached only if the running mass msm_s at low scale is ms(0.5m_s(\sim 0.5 GeV)=170200= 170 - 200 MeV. Our results follow from the analytical expression for the pseudoscalar decay constant fPf_{\rm P} based on the path-integral representation of the meson Green's function.

Keywords

Cite

@article{arxiv.hep-ph/0702229,
  title  = {The running mass $m_s$ at low scalefrom the heavy-light meson decay constants},
  author = {A. M. Badalian and B. L. G. Bakker},
  journal= {arXiv preprint arXiv:hep-ph/0702229},
  year   = {2015}
}

Comments

6 pages, no figures; revtex4