S. Güsken
University of Wuppertal
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Featured researches published by S. Güsken.
Physics Letters B | 1989
S. Güsken; U. Löw; K.H. Mütter; R. Sommer; Apoorva Patel; K. Schilling
We calculate in the quenched approximation the F and D parameters characterising the axial vector matrix elements of the baryon octet. The use of an improved fermion action and smeared interpolating fields enables us to go down in quark mass to the SU ( 3 ) symmetric point. Both the F/D ratio and g A are in good agreement with the experimental values within a statistical error of a≈10%.
Nuclear Physics B - Proceedings Supplements | 1990
S. Güsken
Abstract We present a systematic study of smearing techniques, applied to increase the overlap of Hadron operators with their ground states. We find that the relevant parameters of the different schemes can be optimized such that the Hadron propagators are dominated by the ground state at time separation t = 1 already.
International Journal of Modern Physics C | 1995
Andreas Frommer; Bertold Nöckel; S. Güsken; Thomas Lippert; K. Schilling
The computational effort in the calculation of Wilson fermion quark propagators in Lattice Quantum Chromodynamics can be considerably reduced by exploiting the Wilson fermion matrix structure in inversion algorithms based on the non-symmetric Lanczos process. We consider two such methods: QMR (quasi minimal residual) and BCG (biconjugate gradients). Based on the decomposition M/κ = 1/κ−D of the Wilson mass matrix, using QMR, one can carry out inversions on a whole trajectory of masses simultaneously, merely at the computational expense of a single propagator computation. In other words, one has to compute the propagator corresponding to the lightest mass only, while all the heavier masses are given for free, at the price of extra storage. Moreover, the symmetry γ5M = M†γ5 can be used to cut the computational effort in QMR and BCG by a factor of two. We show that both methods then become — in the critical regime of small quark masses — competitive to BiCGStab and significantly better than the standard MR m...
Physical Review D | 1998
N. Eicker; P. Lacock; K. Schilling; A. Spitz; U. Glässner; S. Güsken; H. Hoeber; Th. Lippert; Th. Struckmann; P. Ueberholz; J. Viehoff; G. Ritzenhöfer
We present the final analysis of the light and strange hadron spectra from a full QCD lattice simulation with two degenerate dynamical sea quark flavors at
Physical Review D | 1999
S. Güsken; K. Schilling; N. Eicker; A. Spitz; Thomas Lippert; Thorsten Struckmann; J. Viehoff; P. Lacock; P. Ueberholz
\ensuremath{\beta}=5.6
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
on a
Physics Letters B | 1996
U. Glässner; S. Güsken; H. Hoeber; Th. Lippert; G. Ritzenhöfer; K. Schilling; G. Siegert; A. Spitz; A. Wachter
{16}^{3}\ifmmode\times\else\texttimes\fi{}32
Physics Letters B | 1988
S. Güsken; K. Schilling; R. Sommer; K.H. Mütter; Apoorva Patel
lattice. Four sets of sea quark masses corresponding to the range
Physical Review D | 1999
A. Spitz; H. Hoeber; N. Eicker; S. Güsken; Th. Lippert; K. Schilling; Thorsten Struckmann; P. Ueberholz; J. Viehoff
0.69l~{m}_{\ensuremath{\pi}}{/m}_{\ensuremath{\rho}}l~0.83
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
are investigated. For reference we also ran a quenched simulation at