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Light and Strange Quark Masses with Dynamical Wilson Fermions
1
Light and Strange Quark Masses with Dynamical Wilson Fermions.
7
9 ∗ a
Henning Hoeber (for the SESAM collaboration )
9
1 aDepartment of Physics, University of Wuppertal, Gaussstr. 20, 42119 Wuppertal, Germany;
p HLRZ c/o J¨ulich Research Centre and DESY, Hamburg, 52425 J¨ulich, Germany.
e
S
We determine the masses of the light and the strange quarks in the MS-scheme using our high-statistics lattice
1 simulation of QCD with dynamical Wilson fermions. For each of our three sea quarks we have analyzed our data
1 at five different values of the valence quark mass, enabling us to parameterize our fit results in the (msea , mvalence)
plane. For the light quark mass we find mlight (2 GeV) = 2.7(2) MeV, which is lower than in quenched simulations.
1 MS
Applying a new method, which we propose to extract the strange quark mass in a sea of two dynamical light
v strange
quarks, we obtain m (2 GeV) = 140(20) MeV.
0 MS
1
3
9 1. Introduction lattice quark mass under consideration. Typi-
0
7 More than 25 years after the introduction of cally, the pseudoscalar meson mass, having the
9 smallest statistical lattice-error of all hadrons, is
/ quarks as the constituents of hadrons the absolute used. This step also invokes χPT, often only to
h values of the light quark masses, as given in the lowest order, to relate the pseudoscalar mass to
p- cur
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