Abstract

We compute the leptonic decay constants fD+f_{D^+}, fDsf_{D_s}, and fK+f_{K^+}, and the quark-mass ratios mc/msm_c/m_s and ms/mlm_s/m_l in unquenched lattice QCD. We use the MILC highly improved staggered quark (HISQ) ensembles with four dynamical quark flavors. Our primary results are fD+=212.6(0.4)(−1.2+1.0) MeVf_{D^+} = 212.6(0.4)({}^{+1.0}_{-1.2})\ \mathrm{MeV}, fDs=249.0(0.3)(−1.5+1.1) MeVf_{D_s} = 249.0(0.3)({}^{+1.1}_{-1.5})\ \mathrm{MeV}, and fDs/fD+=1.1712(10)(−32+29)f_{D_s}/f_{D^+} = 1.1712(10)({}^{+29}_{-32}), where the errors are statistical and total systematic, respectively. We also obtain fK+/fπ+=1.1956(10)(−18+26)f_{K^+}/f_{π^+} = 1.1956(10)({}^{+26}_{-18}), updating our previous result, and determine the quark-mass ratios ms/ml=27.35(5)(−7+10)m_s/m_l = 27.35(5)({}^{+10}_{-7}) and mc/ms=11.747(19)(−43+59)m_c/m_s = 11.747(19)({}^{+59}_{-43}). When combined with experimental measurements of the decay rates, our results lead to precise determinations of the CKM matrix elements ∣Vus∣=0.22487(51)(29)(20)(5)|V_{us}| = 0.22487(51) (29)(20)(5), ∣Vcd∣=0.217(1)(5)(1)|V_{cd}|=0.217(1) (5)(1) and ∣Vcs∣=1.010(5)(18)(6)|V_{cs}|= 1.010(5)(18)(6), where the errors are from this calculation of the decay constants, the uncertainty in the experimental decay rates, structure-dependent electromagnetic corrections, and, in the case of ∣Vus∣|V_{us}|, the uncertainty in ∣Vud∣|V_{ud}|, respectively.

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