ar X iv : h ep - p h / 01 11 22 5 v 1 1 9 N ov 2 00 1 Two - dimensional QCD in the Coulomb gauge

ar X iv : h ep - p h / 01 11 04 9 v 1 6 N ov 2 00 1 The QCD Phase Diagram and Explosive Astrophysics

ar X iv : h ep - t h / 05 11 10 5 v 1 9 N ov 2 00 5 QCD partition function in the external field in the covariant gauge

The QCD partition function in the external stationary gluomag-netic field is computed in the third order in external field invariants in arbitrary dimension and arbitrary covariant gauge. The contributions proportional to third order invariants in gluon field strength are shown to be dependent on covariant quantum gauge fixing parameter α.

ar X iv : h ep - p h / 01 11 07 2 v 2 8 N ov 2 00 1 The φa 0 γ - and φσγ - vertices in light cone QCD

ar X iv : h ep - p h / 01 11 34 1 v 1 2 7 N ov 2 00 1 TUW - 01 - 30 HARD THERMAL LOOPS AND QCD THERMODYNAMICS

These lectures give an introduction to thermal perturbation theory, hard thermal loops, and their use in a nonperturbative, approximately self-consistent resummation of the thermodynamical potentials of quantum chromodynamics.

ar X iv : h ep - t h / 03 11 17 1 v 1 1 9 N ov 2 00 3 Distributions of Dirac Operator Eigenvalues

The distribution of individual Dirac eigenvalues is derived by relating them to the density and higher eigenvalue correlation functions. The relations are general and hold for any gauge theory coupled to fermions under certain conditions which are stated. As a special case, we give examples of the lowest-lying eigenvalue distributions for QCD-like gauge theories without making use of earlier re...