Stefan Schaefer
Humboldt University of Berlin
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Publication
Featured researches published by Stefan Schaefer.
Nuclear Physics | 2011
Stefan Schaefer; Rainer Sommer; Francesco Virotta
Abstract We study the critical slowing down towards the continuum limit of lattice QCD simulations with Hybrid Monte Carlo type algorithms. In particular for the squared topological charge we find it to be very severe with an effective dynamical critical exponent of about 5 in pure gauge theory. We also consider Wilson loops which we can demonstrate to decouple from the modes which slow down the topological charge. Quenched observables are studied and a comparison to simulations of full QCD is made. In order to deal with the slow modes in the simulation, we propose a method to incorporate the information from slow observables into the error analysis of physical observables and arrive at safer error estimates.
Nuclear Physics | 2004
Christof Gattringer; Meinulf Göckeler; Peter Hasenfratz; S. Hauswirth; Kieran Holland; Thomas Jörg; K.J. Juge; C. B. Lang; Ferenc Niedermayer; P.E.L. Rakow; Stefan Schaefer; A. Schäfer
Abstract We present results from quenched spectroscopy calculations with the parametrized fixed-point and the chirally improved Dirac operators. Both these operators are approximate solutions of the Ginsparg–Wilson equation and have good chiral properties. This allows us to work at small quark masses and we explore pseudoscalar-mass to vector-mass ratios down to 0.28. We discuss meson and baryon masses, their scaling properties, finite volume effects and compare our results with recent large scale simulations. We find that the size of quenching artifacts of the masses is strongly correlated with their experimentally observed widths and that the gauge and hadronic scales are consistent.
Journal of High Energy Physics | 2015
Mattia Bruno; D. Djukanovic; Georg P. Engel; Anthony Francis; Gregorio Herdoiza; Hanno Horch; Piotr Korcyl; T. Korzec; Mauro Papinutto; Stefan Schaefer; Enno E. Scholz; Jakob Simeth; Hubert Simma; Wolfgang Söldner
A bstractWe describe a new set of gauge configurations generated within the CLS effort. These ensembles have Nf = 2 + 1 flavors of non-perturbatively improved Wilson fermions in the sea with the Lüscher-Weisz action used for the gluons. Open boundary conditions in time are used to address the problem of topological freezing at small lattice spacings and twisted-mass reweighting for improved stability of the simulations. We give the bare parameters at which the ensembles have been generated and how these parameters have been chosen. Details of the algorithmic setup and its performance are presented as well as measurements of the pion and kaon masses alongside the scale parameter t0.
Journal of High Energy Physics | 2007
Anna Hasenfratz; Roland Hoffmann; Stefan Schaefer
We investigate a variant of hypercubic gauge link smearing where the SU(3) projection is replaced with a normalization to the corresponding unitary group. This smearing is differentiable and thus suitable for use in dynamical fermion simulations using molecular dynamics type algorithms. We show that this smearing is as efficient as projected hypercubic smearing in removing ultraviolet noise from the gauge fields. We test the normalized hypercubic smearing in dynamical improved (clover) Wilson and valence overlap simulations.
Physical Review D | 2002
Christof Gattringer; Roland Hoffmann; Stefan Schaefer
We study the quark-antiquark potential of quenched SU(3) lattice gauge theory with the Luescher-Weisz action. After blocking the gauge fields with the recently proposed hypercubic transformation we compute the Sommer parameter, extract the lattice spacing a and set the scale at 6 different values of the gauge coupling in a range from a = 0.084 fm to 0.136 fm.
Computer Physics Communications | 2004
Thomas DeGrand; Stefan Schaefer
We describe and test a method to compute Euclidean meson two-point functions in lattice QCD. The contribution from the low-lying eigenmodes of the Dirac operator is averaged over all positions of the quark sources. The contribution from the higher modes is estimated in the traditional way with one or a few source points per lattice. In some channels, we observe a significant improvement in the two-point functions for small quark masses.
Physical Review D | 2005
Thomas DeGrand; Stefan Schaefer
We discuss the impact of various improvements on simulations of dynamical overlap fermions using the Hybrid Monte Carlo algorithm. We focus on the usage of fat links and multiple pseudofermion fields.
Journal of High Energy Physics | 2014
Mattia Bruno; Stefan Schaefer; Rainer Sommer
A bstractWe present a measurement of the topological susceptibility in two flavor QCD. In this observable, large autocorrelations are present and also sizable cutoff effects have to be faced in the continuum extrapolation. Within the statistical accuracy of the computation, the result agrees with the expectation from leading order chiral perturbation theory.
arXiv: High Energy Physics - Lattice | 2011
Marina Marinkovic; Stefan Schaefer
Mass preconditioned HMC and DD-HMC are among the most popular algorithms to simulate Wilson fermions. We present a comparison of the performance of the two algorithms for realistic quark masses and lattice sizes. In particular, we use the loc ally deflated solver of the DD-HMC environment also for the mass preconditioned simulations.
Nuclear Physics | 2003
Christof Gattringer; Stefan Schaefer
Abstract We probe the SU (3) vacuum using eigenvectors of the Dirac operator with an arbitrary phase for the temporal boundary condition. We consider configurations with topological charge | Q |=1 near the QCD phase transition and at low temperatures on a torus. For all our ensembles we show that the zero mode of the Dirac operator changes its position as one changes the phase of the boundary condition. For ensembles near the QCD phase transition our results closely resemble the behavior of zero modes for Kraan–van Baal solutions of the classical Yang–Mills equations where the individual lumps are interpreted as monopoles. Our findings near T c and on the torus show that for both cases an excitation with topological charge | Q |=1 is built from several separate lumps.