We theoretically show that moderate interaction between electrons confined to
move in a plane and localized magnetic moments leads to formation of a
noncoplanar magnetic state. The state is similar to the skyrmion crystal
recently observed in cubic systems with the Dzyaloshinskii-Moriya interaction;
however, it does not require spin-orbit interaction. The non-coplanar magnetism
is accompanied by the ground-state electrical and spin currents, generated via
the real-space Berry phase mechanism. We examine the stability of the state
with respect to lattice discreteness effects and the magnitude of magnetic
exchange interaction. The state can be realized in a number of transition metal
and magnetic semiconductor systems