Because present Monte Carol algorithms for lattice QCD may become trapped in a given topological charge sector when one approaches the continuum limit, it is important to understand the effect of calculating at fixed topology. In this work, we show that although the restriction to a fixed topological sector becomes irrelevant in the infinite volume limit, it gives rise to characteristic finite size effects due to contributions from all $\theta$-vacua. We calculate these effects and show how to extract physical results from numerical data obtained at fixed topology
The possibility is explored to relate confinement to properties of gauge invariant field strength co...
We show that, if the formula for the topological charge density operator suggested by fermions obeyi...
Quantum effects of bulk matter, in the form of massive fermions, are considered in the Randall-Sundr...
The monopole order parameter of QCD is computed in terms of gauge invariant field strength correlato...
Topology on the lattice is reviewed. In quenched QCD topological susceptibility chi is fully underst...
The status of topology on the lattice is reviewed. Recent results show that the topological suscepti...
Cooled down and diluted quark-gluon matter is considered. A possibility of condensation of multiquar...
We investigate the topological properties of the SU(3) pure gauge theory by performing numerical sim...
Some results of test runs on a $6^3\times 12$ lattice with Wilson quarks and gauge group SU(2) for a...
The Debye mass m_D is computed nonperturbatively in the deconfined phase of QCD, where chromomagneti...
Following the strategy developed by the ALPHA collaboration, we present a method to compute non-pert...
We determine, by numerical simulations on a lattice, the gauge-invariant two-point correlation funct...
In quenched lattice QCD with standard Wilson fermions the quark propagator is computed very close to...
We study the phase diagram of quark matter at finite temperature (T) and chemical potential (mu) in ...
A linear increase with the volume of the topological susceptibility can signal spontaneous breaking ...
The possibility is explored to relate confinement to properties of gauge invariant field strength co...
We show that, if the formula for the topological charge density operator suggested by fermions obeyi...
Quantum effects of bulk matter, in the form of massive fermions, are considered in the Randall-Sundr...
The monopole order parameter of QCD is computed in terms of gauge invariant field strength correlato...
Topology on the lattice is reviewed. In quenched QCD topological susceptibility chi is fully underst...
The status of topology on the lattice is reviewed. Recent results show that the topological suscepti...
Cooled down and diluted quark-gluon matter is considered. A possibility of condensation of multiquar...
We investigate the topological properties of the SU(3) pure gauge theory by performing numerical sim...
Some results of test runs on a $6^3\times 12$ lattice with Wilson quarks and gauge group SU(2) for a...
The Debye mass m_D is computed nonperturbatively in the deconfined phase of QCD, where chromomagneti...
Following the strategy developed by the ALPHA collaboration, we present a method to compute non-pert...
We determine, by numerical simulations on a lattice, the gauge-invariant two-point correlation funct...
In quenched lattice QCD with standard Wilson fermions the quark propagator is computed very close to...
We study the phase diagram of quark matter at finite temperature (T) and chemical potential (mu) in ...
A linear increase with the volume of the topological susceptibility can signal spontaneous breaking ...
The possibility is explored to relate confinement to properties of gauge invariant field strength co...
We show that, if the formula for the topological charge density operator suggested by fermions obeyi...
Quantum effects of bulk matter, in the form of massive fermions, are considered in the Randall-Sundr...