Add to ORKGWe present results of numerical solutions of Schwinger-Dyson equations for the finite-temperature quark and electron propagators. It is shown that both strongly coupled QED and QCD undergo a chiral symmetry restoring phase transition as the temperature is increased. We go beyond the bare vertex or "rainbow" approximation by applying the finite-temperature Ward-Takahashi identity to constrain the non-perturbative vertex function
Using Mandelstam's approximation to the gluon Dyson-Schwinger equation = we calculate the gluon self...
We present the perturbative QCD calculation of diffractive $D_s$ production in charged current deep ...
A simple but effective method for regularization-renormalization (R-R) is proposed for handling the ...
Strong hadronic decays are discussed in the 't Hooft model for the two-dimensional QCD in the limit ...
The Global Colour Model (GCM) of QCD is a very successful model. Not only is it formally derivable f...
The transition form factor, decay width and charge form factor of pion are calculated within the mod...
The equation of state for quark-gluon plasma is obtained, being valid for arbitrary values of the co...
We study the phase diagram of quark matter at finite temperature (T) and chemical potential (mu) in ...
To describe pion as a bound state of two quark, when their current masses are non equal to zero, is ...
The Debye mass m_D is computed nonperturbatively in the deconfined phase of QCD, where chromomagneti...
We study the chiral phase transition at $T \neq 0$ in the dual Ginzburg-Landau theory using the Schw...
We investigate the interplay of chiral and heavy quark symmetries by using the NJL quark model. Heav...
Two dimensional QCD is quantized on the light front coordinate. We solve the Einstein-Schrödinger eq...
Deconfinement phase transition due to disappearance of confining colorelectric field correlators is ...
The generating functional of heavy baryon chiral perturbation theory at order {\cal O}(Q^2) in the m...
Using Mandelstam's approximation to the gluon Dyson-Schwinger equation = we calculate the gluon self...
We present the perturbative QCD calculation of diffractive $D_s$ production in charged current deep ...
A simple but effective method for regularization-renormalization (R-R) is proposed for handling the ...
Strong hadronic decays are discussed in the 't Hooft model for the two-dimensional QCD in the limit ...
The Global Colour Model (GCM) of QCD is a very successful model. Not only is it formally derivable f...
The transition form factor, decay width and charge form factor of pion are calculated within the mod...
The equation of state for quark-gluon plasma is obtained, being valid for arbitrary values of the co...
We study the phase diagram of quark matter at finite temperature (T) and chemical potential (mu) in ...
To describe pion as a bound state of two quark, when their current masses are non equal to zero, is ...
The Debye mass m_D is computed nonperturbatively in the deconfined phase of QCD, where chromomagneti...
We study the chiral phase transition at $T \neq 0$ in the dual Ginzburg-Landau theory using the Schw...
We investigate the interplay of chiral and heavy quark symmetries by using the NJL quark model. Heav...
Two dimensional QCD is quantized on the light front coordinate. We solve the Einstein-Schrödinger eq...
Deconfinement phase transition due to disappearance of confining colorelectric field correlators is ...
The generating functional of heavy baryon chiral perturbation theory at order {\cal O}(Q^2) in the m...
Using Mandelstam's approximation to the gluon Dyson-Schwinger equation = we calculate the gluon self...
We present the perturbative QCD calculation of diffractive $D_s$ production in charged current deep ...
A simple but effective method for regularization-renormalization (R-R) is proposed for handling the ...