  We demonstrate the importance of the Kondo effect in artificially created
{\it f}-electron superlattices. We show that the Kondo effect does not only
change the density of states of the {\it f}-electron layers, but is also the
cause of pronounced resonances at the Fermi energy in the density of states of
the non-interacting layers in the superlattice, which are between the {\it
f}-electron layers. Remarkably, these resonances strongly depend on the
structure of the superlattice; due to interference, the density of states at
the Fermi energy can be strongly enhanced or even shows no changes at all.
Furthermore, we show that by inserting the Kondo lattice layer into a
three-dimensional (3D) metal, the gap of the Kondo insulating state changes
from a full gap to a pseudo gap with quadratically vanishing spectral weight
around the Fermi energy. Due to the formation of the Kondo insulating state in
the {\it f}-electron layer, the superlattice becomes strongly anisotropic below
the Kondo temperature. We prove this by calculating the in-plane and
out-of-plane conductivity of the superlattice.
