The magnetic susceptibility of a degenerate relativistic Fermi gas is obtained for charged fermions with anomalous magnetic moments. Magnetic properties of the relativistic Fermi gas are of interest because degenerate relativistic electrons and nucleons form white dwarfs and neutron stars.
In this paper we have calculated the exact expression for the magnetic moment of a Fermi gas in a magnetic field (magnetized Fermi gas). The susceptibility obtained from our result becomes the classical Curie-Langevin law in the weak-field limit for a nondegenerate and nonrelativistic gas. The induced magnetic moment M was found to be proportional to the square of the electron density, but at higher densities M passes through a maximum and eventually becomes negative; hence a magnetized gas is first paramagnetic but later becomes diamagnetic. We have also shown that spontaneous magnetization cannot take place in a noninteracting electron gas.
By considering strict relativistic energy of single particle and using the methods of quantum statistics, the relativistic paramagnetism of a weakly interacting Fermi gas in a weak magnetic field is studied, and the relativistic most probable paramagnetic susceptibility as well as the average magnetic susceptibility of the system are solved. On the basis, the influences of relativistic effect on the most probable paramagnetic susceptibility of the system are discussed, and the relativistic critical value of particle number is given. It is shown that, comparing with nonrelativistic situation, when T≫TF, the relativistic most probable magnetic susceptibility and the relativistic critical value of particle number have not changed. When T≪TF, the relativistic effects make the system display paramagnetism easily and susceptibility increase, but the relativistic effects also amplified the impact of the interaction on the magnetic susceptibility.
We discuss the bosonization of a relativistic very dense Fermi gas in a magnetic field and the consequent Bose–Einstein condensation of the resulting relativistic vector gas of charged particles. The model may be applied to paired spin-up electrons. We show that such systems may maintain self-consistently magnetic fields of order 10 10 −10 13 G. That pairing could be the origin of large magnetic fields in some white dwarfs and neutron stars. For fields large enough (~10 13 for white dwarfs), the system becomes unstable and collapses.
By considering strict relativistic energy of single particle and using the methods of quantum statistics,the relativistic paramagnetism of a weakly interacting Fermi gas in a weak magnetic filed is studied,and the relativistic most probable paramagnetic susceptibility as well as the average magnetic susceptibility of the system are solved.On the basis,the influences of relativistic effect on the most probable paramagnetic susceptibility of the system are discussed,and the relativistic critical value of particle number is given.It is shown that,comparing with nonrelativistic situation,when TT_F,the relativistic most probable magnetic susceptibility and the relativistic critical value of particle number have not changed.When TT_F,the relativistic effects make the system display paramagnetism easily and susceptibility increase,but the relativistic effects also amplified the impact of the interaction on the magnetic susceptibility.