We report on a high statistics simulation of SU(2) pure gauge field theory at finite temperature, using the Symanzik action. We determine the critical coupling for the deconfinement phase transition on lattices up to 8 × 24, using finite size scaling techniques. We find that the pattern of asymptotic scaling violation is essentially the same as the one observed with conventional, not improved action. On the other hand, the use of effective couplings defined in terms of plaquette expectation values shows a precocious scaling, with respect to an analogous analysis of data obtained by the use of the Wilson action, which we interpret as an effect of improvement
We report on the determination of the deconfining temperature in SU(3) pure gauge theory, using the ...
We report on the determination of the deconfining temperature in SU(3) pure gauge theory, using the ...
We investigated the finite temperature (T) phase transition for SU(Nc) gauge theory with Nc=4, 6, 8 ...
We report on a high statistics simulation of SU(2) pure gauge field theory at finite temperature, us...
We report on a high statistics simulation of SU(2) pure gauge field theory at finite temperature, us...
We report on a high statistics simulation of SU(2) pure gauge field theory at finite temperature, us...
We report on a high statistics simulation of SU(2) pure gauge field theory at finite temperature, us...
A simulation of the SU(2) theory at finite temperatures by means of a Symanzik improved action is pr...
A simulation of the SU(2) theory at finite temperatures by means of a Symanzik improved action is pr...
A simulation of the SU(2) theory at finite temperatures by means of a Symanzik improved action is pr...
A simulation of the SU(2) theory at finite temperatures by means of a Symanzik improved action is pr...
A simulation of the SU(2) theory at finite temperatures by means of a Symanzik improved action is pr...
Fingberg J, Heller UM, Karsch F. Scaling and asymptotic scaling in the SU(2) gauge theory. Nuclear P...
We report on the determination of the deconfining temperature in SU(3) pure gauge theory, using the ...
We report on the determination of the deconfining temperature in SU(3) pure gauge theory, using the ...
We report on the determination of the deconfining temperature in SU(3) pure gauge theory, using the ...
We report on the determination of the deconfining temperature in SU(3) pure gauge theory, using the ...
We investigated the finite temperature (T) phase transition for SU(Nc) gauge theory with Nc=4, 6, 8 ...
We report on a high statistics simulation of SU(2) pure gauge field theory at finite temperature, us...
We report on a high statistics simulation of SU(2) pure gauge field theory at finite temperature, us...
We report on a high statistics simulation of SU(2) pure gauge field theory at finite temperature, us...
We report on a high statistics simulation of SU(2) pure gauge field theory at finite temperature, us...
A simulation of the SU(2) theory at finite temperatures by means of a Symanzik improved action is pr...
A simulation of the SU(2) theory at finite temperatures by means of a Symanzik improved action is pr...
A simulation of the SU(2) theory at finite temperatures by means of a Symanzik improved action is pr...
A simulation of the SU(2) theory at finite temperatures by means of a Symanzik improved action is pr...
A simulation of the SU(2) theory at finite temperatures by means of a Symanzik improved action is pr...
Fingberg J, Heller UM, Karsch F. Scaling and asymptotic scaling in the SU(2) gauge theory. Nuclear P...
We report on the determination of the deconfining temperature in SU(3) pure gauge theory, using the ...
We report on the determination of the deconfining temperature in SU(3) pure gauge theory, using the ...
We report on the determination of the deconfining temperature in SU(3) pure gauge theory, using the ...
We report on the determination of the deconfining temperature in SU(3) pure gauge theory, using the ...
We investigated the finite temperature (T) phase transition for SU(Nc) gauge theory with Nc=4, 6, 8 ...