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Charm quark system at the physical point of 2+1 flavor lattice QCD

Abstract

We investigate the charm quark system using the relativistic heavy quark action on 2+1 flavor PACS-CS configurations previously generated on 323×6432^3 \times 64 lattice. The dynamical up-down and strange quark masses are set to the physical values by using the technique of reweighting to shift the quark hopping parameters from the values employed in the configuration generation. At the physical point, the lattice spacing equals a1=2.194(10)a^{-1}=2.194(10) GeV and the spatial extent L=2.88(1)L=2.88(1) fm. The charm quark mass is determined by the spin-averaged mass of the 1S charmonium state, from which we obtain m_{\rm charm}^{\msbar}(\mu = m_{\rm charm}^{\msbar}) = 1.260(1)(6)(35) GeV, where the errors are due to our statistics, scale determination and renormalization factor. An additional systematic error from the heavy quark is of order αs2f(mQa)(aΛQCD)\alpha_s^2 f(m_Q a)(a \Lambda_{QCD}), which is estimated to be a percent level if the factor f(mQa)f(m_Q a) analytic in mQam_Q a is of order unity. Our results for the charmed and charmed-strange meson decay constants are fD=226(6)(1)(5)f_D=226(6)(1)(5) MeV, fDs=257(2)(1)(5)f_{D_s}=257(2)(1)(5) MeV, again up to the heavy quark errors of order αs2f(mQa)(aΛQCD)\alpha_s^2 f(m_Q a)(a \Lambda_{QCD}). Combined with the CLEO values for the leptonic decay widths, these values yield Vcd=0.205(6)(1)(5)(9)|V_{cd}| = 0.205(6)(1)(5)(9), Vcs=1.00(1)(1)(3)(3)|V_{cs}| = 1.00(1)(1)(3)(3), where the last error is on account of the experimental uncertainty of the decay widths.Comment: 16 pages, 12 figure

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