The non-perturbative input necessary for the determination of the ${\cal O}(g^6)$ part of the weak coupling expansion of the free energy density for SU(2) and SU(3) gauge theories is estimated. Although the perturbative information completing the contribution to this order is missing, we give arguments that the magnetic fluctuations are dominated by screened elementary magnetic gluons
We discuss the logarithmic contributions to the vacuum energy density of the three-dimensional SU(3)...
The cancellation of perturbative contributions to the string tension in gluodynamics in the framewor...
The QGP (Quark Gluon Plasma) is thought to have lled the Universe in its early stages. For this reas...
Lütgemeier M, Karsch F, Patkos A, Rank J. The non-perturbative O(g(6)) contribution to the free ener...
Karsch F, Lütgemeier M, Patkos A, Rank J. The O(g(6)) coefficient in the thermodynamic potential of ...
It is determined that the total perturbative contribution to the free-energy of hot SU(3) gauge theo...
We use high precision lattice simulations to calculate the plaquette expectation value in three-dime...
The hot electroweak potential for small Higgs field values is argued to obtain contributions from a ...
We calculate electric and magnetic masses of gluons between T = T_c and 6T_c using lattice QCD (quan...
Perturbation theory for non-abelian gauge theories at finite temperature is plagued by infrared div...
The divergent perturbative expansion of the free-energy density of thermal SU(3) gauge theory is res...
According to a proposal by Arnold and Yaffe, the non-perturbative g^2T-contribution to the Debye mas...
The conventional weak-coupling expansion for the pressure of a hot plasma shows no sign of convergen...
We compute the free energy density F for gauge theories, with fermions, at high temperature and zero...
Philipsen O, Bieletzki D, Schroeder Y. Screened perturbation theory for 3d Yang-Mills theory and the...
We discuss the logarithmic contributions to the vacuum energy density of the three-dimensional SU(3)...
The cancellation of perturbative contributions to the string tension in gluodynamics in the framewor...
The QGP (Quark Gluon Plasma) is thought to have lled the Universe in its early stages. For this reas...
Lütgemeier M, Karsch F, Patkos A, Rank J. The non-perturbative O(g(6)) contribution to the free ener...
Karsch F, Lütgemeier M, Patkos A, Rank J. The O(g(6)) coefficient in the thermodynamic potential of ...
It is determined that the total perturbative contribution to the free-energy of hot SU(3) gauge theo...
We use high precision lattice simulations to calculate the plaquette expectation value in three-dime...
The hot electroweak potential for small Higgs field values is argued to obtain contributions from a ...
We calculate electric and magnetic masses of gluons between T = T_c and 6T_c using lattice QCD (quan...
Perturbation theory for non-abelian gauge theories at finite temperature is plagued by infrared div...
The divergent perturbative expansion of the free-energy density of thermal SU(3) gauge theory is res...
According to a proposal by Arnold and Yaffe, the non-perturbative g^2T-contribution to the Debye mas...
The conventional weak-coupling expansion for the pressure of a hot plasma shows no sign of convergen...
We compute the free energy density F for gauge theories, with fermions, at high temperature and zero...
Philipsen O, Bieletzki D, Schroeder Y. Screened perturbation theory for 3d Yang-Mills theory and the...
We discuss the logarithmic contributions to the vacuum energy density of the three-dimensional SU(3)...
The cancellation of perturbative contributions to the string tension in gluodynamics in the framewor...
The QGP (Quark Gluon Plasma) is thought to have lled the Universe in its early stages. For this reas...