“…( 18) and ( 19) are in agreement with the recent extensive lattice QCD calculations of the quark masses performed by using Wilson fermions in the quenched approximation [20]- [22]. They are also in good agreement with the current lattice world averages, presented in the reviews [6,7] and in the 2002 Review of Particle Physics [23]. The main feature of the present study is, in our opinion, the special attention dedicated to the reduction and control of the systematic uncertainties within the quenched approximation.…”
Section: Systematic Uncertainties and Final Resultssupporting
confidence: 88%
“…in good agreement with the current lattice world averages [6,7]. For the ratio of the strange to the average light quark mass we find…”
Section: Introductionsupporting
confidence: 87%
“…where the bare axial current is improved at O(a) as 5) and (7), are only functions of the bare lattice coupling g 2 0 .…”
Section: Details Of the Lattice Calculationmentioning
confidence: 99%
“…For each value of the hopping parameter, we also present in table 2 the corresponding values of the VWI and AWI quark masses, defined in eqs. ( 5) and (7), renormalized in the RI/MOM scheme at the scale µ = 3 GeV.…”
Section: Details Of the Lattice Calculationmentioning
We compute the strange and the average up/down quark masses in the quenched approximation of lattice QCD, by using the O(a)-improved Wilson action and operators and implementing the non-perturbative renormalization. Our computation is performed at four values of the lattice spacing, from which we could extrapolate to the continuum limit. Our final result for the strange quark mass is m(s)((MS) over bar) (2 GeV) = (106 +/- 2 +/- 8) MeV. For the average up/down quark mass we obtain m(l)((MS) over bar) (2 GeV) = (4.4 +/- 0.1 +/- 0.4) MeV and the ratio m(s)/m(l) = (24.3 +/- 0.2 +/- 0.6). (C) 2003 Elsevier Science B.V. All rights reserved
“…( 18) and ( 19) are in agreement with the recent extensive lattice QCD calculations of the quark masses performed by using Wilson fermions in the quenched approximation [20]- [22]. They are also in good agreement with the current lattice world averages, presented in the reviews [6,7] and in the 2002 Review of Particle Physics [23]. The main feature of the present study is, in our opinion, the special attention dedicated to the reduction and control of the systematic uncertainties within the quenched approximation.…”
Section: Systematic Uncertainties and Final Resultssupporting
confidence: 88%
“…in good agreement with the current lattice world averages [6,7]. For the ratio of the strange to the average light quark mass we find…”
Section: Introductionsupporting
confidence: 87%
“…where the bare axial current is improved at O(a) as 5) and (7), are only functions of the bare lattice coupling g 2 0 .…”
Section: Details Of the Lattice Calculationmentioning
confidence: 99%
“…For each value of the hopping parameter, we also present in table 2 the corresponding values of the VWI and AWI quark masses, defined in eqs. ( 5) and (7), renormalized in the RI/MOM scheme at the scale µ = 3 GeV.…”
Section: Details Of the Lattice Calculationmentioning
We compute the strange and the average up/down quark masses in the quenched approximation of lattice QCD, by using the O(a)-improved Wilson action and operators and implementing the non-perturbative renormalization. Our computation is performed at four values of the lattice spacing, from which we could extrapolate to the continuum limit. Our final result for the strange quark mass is m(s)((MS) over bar) (2 GeV) = (106 +/- 2 +/- 8) MeV. For the average up/down quark mass we obtain m(l)((MS) over bar) (2 GeV) = (4.4 +/- 0.1 +/- 0.4) MeV and the ratio m(s)/m(l) = (24.3 +/- 0.2 +/- 0.6). (C) 2003 Elsevier Science B.V. All rights reserved
“…The input we use for qq χ is the value derived from sum rules in Ref. [19], which is in agreement with most recent sum rules determinations of this condensate and of light quark masses -see [20] for instance-and the lattice light quark masses world average in [21]. The value of F 0 is from Ref.…”
This paper discusses a general class of ladder resummation inspired hadronic approximations. It is found that this approach naturally reproduces many successes of single meson per channel saturation models (e.g. VMD) and NJL based models. In particular the existence of a constituent quark mass and a gap equation follows naturally. We construct an approximation that satisfies a large set of QCD shortdistance and large N c constraints and reproduces many hadronic observables.We show how there exists in general a problem between QCD short-distance constraints for Green Functions and those for form factors and cross-sections following from the quark-counting rule. This problem while expected for Green functions that do not vanish in purely perturbative QCD also persists for many Green functions that are order parameters.
We compute the b quark mass from dynamical lattice QCD with clover quarks.
The calculation is done at a fixed lattice spacing with sea quark masses as low
as half the strange quark mass. Our final result is m_b(m_b} = 4.25(2)(11) GeV,
where the first error is statistical and the last error is the systematic
uncertainty.Comment: 10 page
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