The covariant propagator of a fermion with intrinsic magnetic moment interacting with a uniform external magnetic field is presented for finite temperature and baryonic density. The case of a scalar boson is also considered. The final expressions are given in terms of a four-dimensional momentum representation. These results, which take account of the full effect of the magnetic field, are used to evaluate the modification of the pion mass at zero temperature as a function of the density and the magnetic intensity. For this purpose a self-consistent calculation, including one- and two-pion vertices, is employed.Instituto de Física La PlataConsejo Nacional de Investigaciones Científicas y Técnica
By extending the $$\Phi $$-derivable approach in the Nambu–Jona-Lasinio model to a finite magnetic f...
By extending the Phi-derivable approach in the Nambu-Jona-Lasinio model to a finite magnetic field w...
AbstractWe investigate the modification of the pion self-energy at finite temperature due to its int...
The covariant propagator of a fermion with intrinsic magnetic moment interacting with a uniform exte...
The covariant propagator of a fermion with intrinsic magnetic moment interacting with a uniform exte...
The covariant propagator of a fermion with intrinsic magnetic moment interacting with a uniform exte...
We obtain the covariant propagator at finite temperature for interacting baryons immersed in a stron...
We obtain the covariant propagator at finite temperature for interacting baryons immersed in a stron...
The effective masses of the neutral mesons in a hadronic medium and under an external magnetic field...
We obtain the covariant propagator at finite temperature for interacting baryons immersed in a stron...
The effective masses of the neutral mesons in a hadronic medium and under an external magnetic field...
The effective masses of the neutral mesons in a hadronic medium and under an external magnetic field...
The effective masses of the neutral mesons in a hadronic medium and under an external magnetic field...
The properties of the neutral pion in quark matter under the influence of an external magnetic field...
With the Nambu-Jona-Lasinio (NJL) model we calculate the properties of pion and sigma-meson at finit...
By extending the $$\Phi $$-derivable approach in the Nambu–Jona-Lasinio model to a finite magnetic f...
By extending the Phi-derivable approach in the Nambu-Jona-Lasinio model to a finite magnetic field w...
AbstractWe investigate the modification of the pion self-energy at finite temperature due to its int...
The covariant propagator of a fermion with intrinsic magnetic moment interacting with a uniform exte...
The covariant propagator of a fermion with intrinsic magnetic moment interacting with a uniform exte...
The covariant propagator of a fermion with intrinsic magnetic moment interacting with a uniform exte...
We obtain the covariant propagator at finite temperature for interacting baryons immersed in a stron...
We obtain the covariant propagator at finite temperature for interacting baryons immersed in a stron...
The effective masses of the neutral mesons in a hadronic medium and under an external magnetic field...
We obtain the covariant propagator at finite temperature for interacting baryons immersed in a stron...
The effective masses of the neutral mesons in a hadronic medium and under an external magnetic field...
The effective masses of the neutral mesons in a hadronic medium and under an external magnetic field...
The effective masses of the neutral mesons in a hadronic medium and under an external magnetic field...
The properties of the neutral pion in quark matter under the influence of an external magnetic field...
With the Nambu-Jona-Lasinio (NJL) model we calculate the properties of pion and sigma-meson at finit...
By extending the $$\Phi $$-derivable approach in the Nambu–Jona-Lasinio model to a finite magnetic f...
By extending the Phi-derivable approach in the Nambu-Jona-Lasinio model to a finite magnetic field w...
AbstractWe investigate the modification of the pion self-energy at finite temperature due to its int...