The perturbation theory in terms of the s-f exchange model is used to analy
ze the problem of a non-Fermi-liquid behavior in two-dimensional (2D) and t
hree-dimensional (3D) antiferromagnetic (AFM) metals. The effects of intera
ction of conduction electrons with spin waves on the electron spectrum, the
rmodynamic properties, and transport properties are considered. At very low
temperatures T < T* similar to (Delta/E-F)T-N, where Delta is the AFM spli
tting of the electron spectrum, a Fermi-liquid behavior is observed; in the
3D case, there are nonanalytic corrections to heat capacity of an order of
T(3)lnT. At T> T*, in the 2D case and in 3D systems in which "nesting" in
the electron spectrum is observed (or anomalies in the magnon spectrum are
present), the physical picture corresponds to the marginal Fermi liquid (of
which the contributions of the TlnT type to the heat capacity and almost l
inear temperature dependence of the resistivity are typical). Contributions
to the resistivity and thermoelectric power due to the interference of spi
n-wave and impurity-related scattering are discussed.