The universality of the continuum limit and the applicability of renormalized perturbation theory are tested in the SU(2) lattice gauge theory by computing two different non-perturbatively defined running couplings over a large range of energies. The lattice data (which were generated on the powerful APE computers at Rome II and DESY) are extrapolated to the continuum limit by simulating sequences of lattices with decreasing spacings. Our results confirm the expected universality at all energies to a precision of a few percent. We find, however, that perturbation theory must be used with care when matching different renormalized couplings at high energies
Following Symanzik we argue that the Schrödinger functional in lattice gauge theories without matter...
Following Symanzik we argue that the Schr\"odinger functional in lattice gauge theories without matt...
and U(1) parts have weak couplings and can be studied accurately with perturbative methods, the SU(3...
The universality of the continuum limit and the applicability of renormalized perturbation theory ar...
We use a massively parallel supercomputer to simulate a 483.56 lattice with SU (2) pure gauge theory...
A perturbative renormalization procedure is proposed which applies to massive field theories on a sp...
Precision tests of QCD perturbation theory are not readily available from experimental data. The mai...
The lattice formulation of Quantum Field Theory (QFT) can be exploited in many ways. We can derive t...
Abstract An extensive study of the compact U(1) lattice gauge theory with a higher derivative gauge-...
AbstractLinear lattice gauge theory is based on link variables that are arbitrary complex or real N×...
Abstract. It is shown that in four space-time dimensions the compact U(l) lattice gauge theory with ...
Using Monte Carlo simulations, we study the phase diagram of a two-parameter action for a SU (2) lat...
The renormalisation group running of the quark mass is determined non-perturbatively for a large ran...
We perform numerical studies of the running coupling constant alpha_R(p^2) and of the gluon and ghos...
We calculate the lowest glueball masses and the string tension for both Manton's action and for Syma...
Following Symanzik we argue that the Schrödinger functional in lattice gauge theories without matter...
Following Symanzik we argue that the Schr\"odinger functional in lattice gauge theories without matt...
and U(1) parts have weak couplings and can be studied accurately with perturbative methods, the SU(3...
The universality of the continuum limit and the applicability of renormalized perturbation theory ar...
We use a massively parallel supercomputer to simulate a 483.56 lattice with SU (2) pure gauge theory...
A perturbative renormalization procedure is proposed which applies to massive field theories on a sp...
Precision tests of QCD perturbation theory are not readily available from experimental data. The mai...
The lattice formulation of Quantum Field Theory (QFT) can be exploited in many ways. We can derive t...
Abstract An extensive study of the compact U(1) lattice gauge theory with a higher derivative gauge-...
AbstractLinear lattice gauge theory is based on link variables that are arbitrary complex or real N×...
Abstract. It is shown that in four space-time dimensions the compact U(l) lattice gauge theory with ...
Using Monte Carlo simulations, we study the phase diagram of a two-parameter action for a SU (2) lat...
The renormalisation group running of the quark mass is determined non-perturbatively for a large ran...
We perform numerical studies of the running coupling constant alpha_R(p^2) and of the gluon and ghos...
We calculate the lowest glueball masses and the string tension for both Manton's action and for Syma...
Following Symanzik we argue that the Schrödinger functional in lattice gauge theories without matter...
Following Symanzik we argue that the Schr\"odinger functional in lattice gauge theories without matt...
and U(1) parts have weak couplings and can be studied accurately with perturbative methods, the SU(3...