2000
DOI: 10.1103/physrevd.62.054504
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Lattice determination of light quark masses

Abstract: A fully non-perturbative lattice determination of the up/down and strange quark masses is given for quenched QCD using both, O(a) improved Wilson fermions and ordinary Wilson fermions. For the strange quark mass with O(a) improved fermions we obtain m M S s (µ = 2 GeV) = 105(4) MeV, using the interquark force scale r 0 . Due to quenching problems fits are only possible for quark masses larger than the strange quark mass. If we extrapolate our fits to the up/down quark mass we find for the average mass m M S l … Show more

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Cited by 35 publications
(33 citation statements)
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“…The four-loop value for ∆ M S S (µ) has been given in [36]. At µ = 2 GeV it is ∆ M S S (2 GeV) = 0.721 (10).…”
Section: Nonperturbative Renormalizationmentioning
confidence: 99%
“…The four-loop value for ∆ M S S (µ) has been given in [36]. At µ = 2 GeV it is ∆ M S S (2 GeV) = 0.721 (10).…”
Section: Nonperturbative Renormalizationmentioning
confidence: 99%
“…data to Eq. (25), we obtain A = 0.617 (11), to be compared to A (BPT) = 0.573, as computed in one-loop (boosted) perturbation theory [33] 8 . According to Eq.…”
Section: Practical Implementationmentioning
confidence: 99%
“…(35) we get the results quoted in Eq. (11). In the calculation of m RGI q and m MS (µ), we have used the physical value of α s (µ), corresponding to α s (M Z ) = 0.118 [38], computed with the appropriate number of active flavors, e.g.…”
Section: Extracting the Physical Quark Massmentioning
confidence: 99%
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“…(Recent n f = 2 + 1 results [7], have finer lattice spacings.) These authors quote strange quark masses of O(80) MeV, lying 15 − 30% below the corresponding quenched results [9,10].…”
Section: Introductionmentioning
confidence: 99%