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A Lattice Determination of Light Quark Masses
High Energy Physics - Lattice · Submitted 5 Aug 1999
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim 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.
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The abstract, sentence by sentence
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 $m^{\msbar}_s(\mu=2 {GeV}) = 105(4) {MeV}$, 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 $m^{\msbar}_l(\mu=2 {GeV}) = 4.4(2) {MeV}$.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | 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. | contribution 0.96 | 0.96 | 0.16 | asserted 1.00 |
| s1 | For the strange quark mass with $O(a)$ improved fermions we obtain $m^{\msbar}_s(\mu=2 {GeV}) = 105(4) {MeV}$, using the interquark force scale $r_0$. | result 1.00 | 0.96 | 0.31 | asserted 1.00 |
| s2 | Due to quenching problems fits are only possible for quark masses larger than the strange quark mass. | limitation 1.00 | 0.58 | 0.04 | asserted 0.97 |
| s3 | If we extrapolate our fits to the up/down quark mass we find for the average mass $m^{\msbar}_l(\mu=2 {GeV}) = 4.4(2) {MeV}$. | result 1.00 | 0.96 | 0.34 | asserted 0.99 |
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The paper
Original 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 $m^{\msbar}_s(\mu=2 {GeV}) = 105(4) {MeV}$, 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 $m^{\msbar}_l(\mu=2 {GeV}) = 4.4(2) {MeV}$.
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1 arXiv paper cite this in 1 sentence
Papers whose main result relates to this one's
States the same result 1 paper
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Our final result for the strange quark mass (in the MSbar scheme) is ms(2 GeV) = (106 +/- 2 +/- 8) MeV.
Continuum Determination of Light Quark Masses from Quenched Lattice QCD · 0.86
Papers citing it
Uses its method or tool 1 paper
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The tree-level on-shell-improved vector renormalization constant can then be obtained by computing [ref] [equation] where $m^W=m^bare-m^crit$.
Scaling study for 2 HEX smeared fermions: hadron and quark masses · Scaling of quenched quark masses · 0.99
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