AbstractThe SU(3) beta function is computed from Wilson loops to 20th order numerical stochastic perturbation theory. An attempt is made to include massless fermions, whose contribution is known analytically to 4th order. The question whether the theory admits an infrared stable fixed point is addressed
Some results of test runs on a $6^3\times 12$ lattice with Wilson quarks and gauge group SU(2) for a...
SU(2) gauge theory with Nf=24 massless fermions is non-interacting at long distances, i.e. it has an...
We study the discrete β function of SU(3) gauge theory with N f = 12 massless fermions in the fundam...
The SU(3) beta function is computed from Wilson loops to 20th order numerical stochastic perturbatio...
AbstractWe prove that the β-function of the Grosse–Wulkenhaar model including a magnetic field vanis...
We compute $\Lambda_{\bar{MS}}$ for two flavors of light dynamical quarks using non-perturbatively $...
The exactly soluble Luttinger model can be also analyzed from the point of view of the renormalizati...
We computed the static potential and Wilson loops to $O(\alpha^2)$ in perturbation theory for differ...
The Gell-Mann -- Low function \beta(g) in QED (g is the fine structure constant) is reconstructed. A...
The potential of a static quark-antiquark pair is studied in the range 0.05 fm $<$ r $<$ 0.8 fm, emp...
We calculate the 3-loop perturbative expansion of the average plaquette in lattice QCD with N_f mass...
The equation for the gluon propagator in the approach of Baker-Ball-Zachariasen is considered. The p...
Infrared finite solutions for the gluon propagator of pure QCD are obtained from the gauge-invariant...
Using Mandelstam's approximation to the gluon Dyson-Schwinger equation = we calculate the gluon self...
We consider NLS on $T^2$ with multiplicative spatial white noise and nonlinearity between cubic and...
Some results of test runs on a $6^3\times 12$ lattice with Wilson quarks and gauge group SU(2) for a...
SU(2) gauge theory with Nf=24 massless fermions is non-interacting at long distances, i.e. it has an...
We study the discrete β function of SU(3) gauge theory with N f = 12 massless fermions in the fundam...
The SU(3) beta function is computed from Wilson loops to 20th order numerical stochastic perturbatio...
AbstractWe prove that the β-function of the Grosse–Wulkenhaar model including a magnetic field vanis...
We compute $\Lambda_{\bar{MS}}$ for two flavors of light dynamical quarks using non-perturbatively $...
The exactly soluble Luttinger model can be also analyzed from the point of view of the renormalizati...
We computed the static potential and Wilson loops to $O(\alpha^2)$ in perturbation theory for differ...
The Gell-Mann -- Low function \beta(g) in QED (g is the fine structure constant) is reconstructed. A...
The potential of a static quark-antiquark pair is studied in the range 0.05 fm $<$ r $<$ 0.8 fm, emp...
We calculate the 3-loop perturbative expansion of the average plaquette in lattice QCD with N_f mass...
The equation for the gluon propagator in the approach of Baker-Ball-Zachariasen is considered. The p...
Infrared finite solutions for the gluon propagator of pure QCD are obtained from the gauge-invariant...
Using Mandelstam's approximation to the gluon Dyson-Schwinger equation = we calculate the gluon self...
We consider NLS on $T^2$ with multiplicative spatial white noise and nonlinearity between cubic and...
Some results of test runs on a $6^3\times 12$ lattice with Wilson quarks and gauge group SU(2) for a...
SU(2) gauge theory with Nf=24 massless fermions is non-interacting at long distances, i.e. it has an...
We study the discrete β function of SU(3) gauge theory with N f = 12 massless fermions in the fundam...