The properties of a slightly nonideal 2D Fermi gas in a magnetic field
are analyzed by a Feynman-diagram technique. Expressions for the eige
nenergy part of the one-particle Green's function are derived in up to
second-order perturbation theory. Because the spectrum of the 2D part
icles is discrete in a magnetic field, there is no attenuation of the
quasiparticles, and there is a splitting of seed Landau levels. The ei
genenergy part has a pole at zero frequency. The maximum filling facto
r for each sublevel is v(max) = 1/2.