Abstract

By combining the first unquenched lattice computation of the B-meson binding energy with the recently calculated two-loop contribution to the lattice HQET mass, we determine the MSˉ\bar{MS} b-quark mass, mˉb(mˉb)\bar{m}_{b}(\bar{m}_{b}) at the NNLO. We find mˉb(mˉb)=(4.26±0.03±0.04±0.05)GeV\bar{m}_{b}(\bar{m}_{b}) = (4.26\pm 0.03 \pm 0.04 \pm 0.05) {\rm GeV}. The inclusion of the two-loop effects is one of the steps necessary to extract mˉb(mˉb)\bar{m}_{b}(\bar{m}_{b}) with a precision better than O(ΛQCD){\cal O}(Λ_{QCD}), which is the uncertainty due to the presence of an IR renormalon singularity in the perturbative series of the residual mass. Our results have been obtained on a sample of 60 lattices of size 243×4024^{3}\times 40 at β=5.6β=5.6, using the unquenched Wilson action with two degenerate sea quarks. The quark propagators have been computed using the unquenched links generated by the TχχL Collaboration.

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