We present first results for a study with two mass-degenerate dynamical Chirally Improved (CI) fermions on lattices of spatial extent 2.4 fm. The CI Dirac operator obeys the Ginsparg-Wilson condition in good approximation. The pion mass we use is still large O(470 MeV) for the 16**3*32 lattices with lattice spacing of 0.15 fm. The hadron masses are obtained with the variational technique and the results compared with earlier quenched calculations with similar lattice parameters. We find indications for the isovector, scalar meson a0(980) near the experimental value, in contradistinction to quenched results which always produced a mass value compatible with the first excitation a0(1450)
We calculate meson and baryon masses in quenched QCD for the small quark masses of phenomenological ...
One of the great challenges of lattice QCD is to produce unambiguous predictions for the properties ...
We extend to quenched QCD an earlier investigation of the chiral structure of the masses of the nucl...
Algorithmic and technical progress achieved over the last few years makes QCD simulations with light...
In this contribution we present results from quenched QCD simulations with the parameterized fixed-p...
7 pages, 9 figures. Talk presented at the XXV International Symposium on Lattice Field Theory, July ...
Light quark masses are calculated in lattice QCD with two degenerate flavors of dynamical quarks. Th...
The Fixed Point Dirac Operator and Chirally Improved Fermions both use large numbers of gauge paths ...
Light quark masses are calculated in lattice QCD with two degenerate flavors of dynamical quarks. Th...
We present excited meson masses from quenched calculations using chirally improved (CI) quarks at pi...
We compare the eigenvalue spectra of the Dirac operator from a simulation with two mass degenerate d...
We present results from quenched spectroscopy calculations with the parametrized fixed-point and the...
We present results for masses of excited mesons from quenched calculations using chirally improved q...
Light quark masses are calculated in lattice QCD with two degenerate flavors of dynamical quarks. Th...
Consideration of the analytic properties of pion-induced baryon self-energies leads to new functiona...
We calculate meson and baryon masses in quenched QCD for the small quark masses of phenomenological ...
One of the great challenges of lattice QCD is to produce unambiguous predictions for the properties ...
We extend to quenched QCD an earlier investigation of the chiral structure of the masses of the nucl...
Algorithmic and technical progress achieved over the last few years makes QCD simulations with light...
In this contribution we present results from quenched QCD simulations with the parameterized fixed-p...
7 pages, 9 figures. Talk presented at the XXV International Symposium on Lattice Field Theory, July ...
Light quark masses are calculated in lattice QCD with two degenerate flavors of dynamical quarks. Th...
The Fixed Point Dirac Operator and Chirally Improved Fermions both use large numbers of gauge paths ...
Light quark masses are calculated in lattice QCD with two degenerate flavors of dynamical quarks. Th...
We present excited meson masses from quenched calculations using chirally improved (CI) quarks at pi...
We compare the eigenvalue spectra of the Dirac operator from a simulation with two mass degenerate d...
We present results from quenched spectroscopy calculations with the parametrized fixed-point and the...
We present results for masses of excited mesons from quenched calculations using chirally improved q...
Light quark masses are calculated in lattice QCD with two degenerate flavors of dynamical quarks. Th...
Consideration of the analytic properties of pion-induced baryon self-energies leads to new functiona...
We calculate meson and baryon masses in quenched QCD for the small quark masses of phenomenological ...
One of the great challenges of lattice QCD is to produce unambiguous predictions for the properties ...
We extend to quenched QCD an earlier investigation of the chiral structure of the masses of the nucl...