G. Siegert
University of Wuppertal
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Featured researches published by G. Siegert.
Physics Letters B | 1997
N. Eicker; U. Glässner; S. Güsken; H. Hoeber; P. Lacock; Th. Lippert; G. Ritzenhöfer; K. Schilling; G. Siegert; A. Spitz; P. Ueberholz; J. Viehoff
We determine the masses of the light and the strange quarks in the
European Physical Journal C | 2000
M. Adams; J. Novak; U. Ecker; A. Röser; C. Halliwell; H.J. Gebauer; D.G. Michael; R.D. Kennedy; Hugh E. Montgomery; V. Eckardt; T. Zhao; C.W. Salgado; S. Wolbers; T. Dreyer; W. Dougherty; Z. Jin; R.W. Finlay; J. Haas; B. Pawlik; K. Olkiewicz; H. G. E. Kobrak; Baker; N. Schmitz; W. Wittek; L.S. Osborne; R.A. Swanson; A. Banerjee; D. F. Geesaman; A. Manz; M. Aderholz
bar{MS}
Physics Letters B | 1996
U. Glässner; S. Güsken; H. Hoeber; Th. Lippert; G. Ritzenhöfer; K. Schilling; G. Siegert; A. Spitz; A. Wachter
-scheme using our high-statistics lattice simulation of QCD with dynamical Wilson fermions. For the light quark mass we find
Physics Letters B | 1996
N. Eicker; U. Glässner; S. Güsken; H. Hoeber; Thomas Lippert; G. Ritzenhöfer; K. Schilling; G. Siegert; A. Spitz; P. Ueberholz; J. Viehoff
m^{light}_{bar{MS}}(2 GeV) = 2.7(2) MeV
arXiv: High Energy Physics - Lattice | 1998
Th. Lippert; Gunnar S. Bali; N. Eicker; L. Giusti; U. Glässner; S. Güsken; H. Hoeber; P. Lacock; G. Martinelli; F. Rapuano; G. Ritzenhöfer; K. Schilling; G. Siegert; A. Spitz; P. Ueberholz; J. Viehoff
, which is lower than in quenched simulations. For the strange quark, in a sea of two dynamical light quarks, we obtain
European Physical Journal C | 1994
Constantia Alexandrou; S. Güsken; F. Jegerlehner; K. Schilling; G. Siegert; Rainer Sommer
m^{strange}_{bar{MS}}(2 GeV) = 140(20) MeV
Physics Letters B | 1994
Constantia Alexandrou; A. Borrelli; S. Güsken; F. Jegerlehner; K. Schilling; G. Siegert; Rainer Sommer
.Abstract We determine the masses of the light and the strange quarks in the MS -scheme using our high-statistics lattice simulation of QCD with dynamical Wilson fermions. For the light quark mass we find m light MS (2 GeV ) = 2.7 (2) MeV , which is lower than in quenched simulations. For the strange quark, in a sea of two dynamical light quarks, we obtain m strange MS (2 GeV ) = 140(20) MeV .
European Physical Journal A | 1997
M. Adams; J. Novak; U. Ecker; P. Madden; C. Halliwell; H.J. Gebauer; H. G. E. Kobrak; K. P. Schüler; D.G. Michael; R.D. Kennedy; Hugh E. Montgomery; V. Eckardt; T. Zhao; C.W. Salgado; S. Wolbers; T. Dreyer; W. Dougherty; Z. Jin; R. Wilson; R.W. Finlay; J. Haas; B. Pawlik; K. Olkiewicz; S. Kaufmann; D.A. Averill; N. Schmitz; J. Seyerlein; A. Röser; L.S. Osborne; R.A. Swanson
We report results of the first measurements of
arXiv: High Energy Physics - Lattice | 1996
S. Güsken; K. Schilling; G. Siegert
Lambda
arXiv: High Energy Physics - Lattice | 1995
Constantia Alexandrou; A. Borrelli; S. Güsken; F. Jegerlehner; K. Schilling; G. Siegert; Rainer Sommer
n and