We study the temperature dependence of the effective bag constant, the mass, and the radius of a nucleon in the formalism of the simple global color symmetry model in the Dyson-Schwinger equation approach of QCD with a Gaussian-type effective gluon propagator. We obtain that, as the temperature is lower than a critical value, the effective bag constant and the mass decrease and the radius increases with the temperature increasing. As the critical temperature is reached, the effective bag constant and the mass vanish and the radius tends to infinity. At the same time, the chiral quark condensate disappears. These phenomena indicate that the deconfinement and the chiral symmetry restoration phase transitions can take place at high temperature...
In the framework of nonlocal SU(2) chiral quark models with Polyakov loop, we analyze the dependence...
Horvatic D, Blaschke D, Klabucar D, Kaczmarek O. Width of the QCD transition in a Polyakov-loop Dyso...
The width of the process π0 → γγ is calculated within effective QCD at finite temperature. We use tw...
Making use of the global color symmetry model (GCM) at finite chemical potential and with a sophisti...
With the global color symmetry model (GCM) being extended to finite chemical potential, the density ...
With the global color symmetry model (GCM) at finite chemical potential, the density dependence of t...
With the global color symmetry model (GCM) being extended to finite chemical potential, the density ...
We study the nucleon at finite temperature using Bethe-Salpeter equation (BSE) where it is considere...
The global colour model at finite temperature is further extended to study the systems at finite che...
With the global color symmetry model being extended to finite chemical potential, we study the densi...
After presenting a brief summary of functional approaches to QCD at vanishing temperatures and densi...
We investigate chiral symmetry restoration in finite spatial volume and at finite temperature by cal...
After introducing essential, qualitative concepts and results, the authors discuss the application o...
With the global color symmetry mode! (GCM) being extended to finite chemical potential, the density ...
We analyze the consequences of the inclusion of the gluonic Polyakov loop in chiral quark models at ...
In the framework of nonlocal SU(2) chiral quark models with Polyakov loop, we analyze the dependence...
Horvatic D, Blaschke D, Klabucar D, Kaczmarek O. Width of the QCD transition in a Polyakov-loop Dyso...
The width of the process π0 → γγ is calculated within effective QCD at finite temperature. We use tw...
Making use of the global color symmetry model (GCM) at finite chemical potential and with a sophisti...
With the global color symmetry model (GCM) being extended to finite chemical potential, the density ...
With the global color symmetry model (GCM) at finite chemical potential, the density dependence of t...
With the global color symmetry model (GCM) being extended to finite chemical potential, the density ...
We study the nucleon at finite temperature using Bethe-Salpeter equation (BSE) where it is considere...
The global colour model at finite temperature is further extended to study the systems at finite che...
With the global color symmetry model being extended to finite chemical potential, we study the densi...
After presenting a brief summary of functional approaches to QCD at vanishing temperatures and densi...
We investigate chiral symmetry restoration in finite spatial volume and at finite temperature by cal...
After introducing essential, qualitative concepts and results, the authors discuss the application o...
With the global color symmetry mode! (GCM) being extended to finite chemical potential, the density ...
We analyze the consequences of the inclusion of the gluonic Polyakov loop in chiral quark models at ...
In the framework of nonlocal SU(2) chiral quark models with Polyakov loop, we analyze the dependence...
Horvatic D, Blaschke D, Klabucar D, Kaczmarek O. Width of the QCD transition in a Polyakov-loop Dyso...
The width of the process π0 → γγ is calculated within effective QCD at finite temperature. We use tw...