We have proven the general relations between the gap equations obeyed by dynamical fermion mass and corresponding effective potentials at finite temperature and chemical potential in D dimensional four-fermion interaction models. This gives an easy approach to get effective potentials directly from the gap equations. We find out explicit expressions for the effective potentials at zero temperature in the cases of $D=2,3$ and 4 for practical use
The Debye mass m_D is computed nonperturbatively in the deconfined phase of QCD, where chromomagneti...
We study resonant Bose-Fermi mixtures at zero temperature, with different relative concentrations of...
Some results of test runs on a $6^3\times 12$ lattice with Wilson quarks and gauge group SU(2) for a...
The catalysis of chiral symmetry breaking in the massless weakly coupled QED in a magnetic field is ...
Dynamical symmetry breaking and the formation of scalar condensates in the SU(2) X U(1) Nambu-Jona-L...
To describe pion as a bound state of two quark, when their current masses are non equal to zero, is ...
We study a two dimensional two species Fermi gas with attractive short-range interactions at zero te...
Two forms are available for the fermion propagator at finite temperature and density. It is shown th...
Quantum effects of bulk matter, in the form of massive fermions, are considered in the Randall-Sundr...
Part fourteen of course materials for Statistical Physics I: PHY525, taught by Gerhard Müller at the...
Using the general form of the static energy solutions to the Dirac equation with a magnetic field, w...
One -loop fermion determinant is discussed for the case in which dynamical chiral symmetry breaking ...
New field content beyond that of the standard model of particle physics can alter the thermal histor...
AbstractThe phase diagram of the Gross–Neveu (GN) model in 2+1 dimensions as a function of chemical ...
The solutions of Heisenberg equations and two-particles eigenvalue problems for nonrelativistic mode...
The Debye mass m_D is computed nonperturbatively in the deconfined phase of QCD, where chromomagneti...
We study resonant Bose-Fermi mixtures at zero temperature, with different relative concentrations of...
Some results of test runs on a $6^3\times 12$ lattice with Wilson quarks and gauge group SU(2) for a...
The catalysis of chiral symmetry breaking in the massless weakly coupled QED in a magnetic field is ...
Dynamical symmetry breaking and the formation of scalar condensates in the SU(2) X U(1) Nambu-Jona-L...
To describe pion as a bound state of two quark, when their current masses are non equal to zero, is ...
We study a two dimensional two species Fermi gas with attractive short-range interactions at zero te...
Two forms are available for the fermion propagator at finite temperature and density. It is shown th...
Quantum effects of bulk matter, in the form of massive fermions, are considered in the Randall-Sundr...
Part fourteen of course materials for Statistical Physics I: PHY525, taught by Gerhard Müller at the...
Using the general form of the static energy solutions to the Dirac equation with a magnetic field, w...
One -loop fermion determinant is discussed for the case in which dynamical chiral symmetry breaking ...
New field content beyond that of the standard model of particle physics can alter the thermal histor...
AbstractThe phase diagram of the Gross–Neveu (GN) model in 2+1 dimensions as a function of chemical ...
The solutions of Heisenberg equations and two-particles eigenvalue problems for nonrelativistic mode...
The Debye mass m_D is computed nonperturbatively in the deconfined phase of QCD, where chromomagneti...
We study resonant Bose-Fermi mixtures at zero temperature, with different relative concentrations of...
Some results of test runs on a $6^3\times 12$ lattice with Wilson quarks and gauge group SU(2) for a...