uniform magnetic field is derived. It is shown that the conductivity is entirely determined by the Chern-Simons coefficient: σij= εijC and that it shows discrete steps as a function of the chemical potential and the magnetic field.
A general expression for the conductivity in the QED2+1 with nonzero fermion density in a uniform magnetic field is derived. It is shown that the conductivity is entirely determined by the Chern-Simons coefficient: σij = εijC and that it shows discrete steps as a function of the chemical potential and the magnetic field.