  Semiclassical chiral fermions manifest the anomalous spin-Hall effect: when
put into a pure electric field they suffer a side jump, analogous to what
happens to their massive counterparts in non-commutative mechanics. The
transverse shift is consistent with the conservation of the angular momentum.
In a pure magnetic field instead, spiraling motion is found. Motion in
Hall-type perpendicular electric and magnetic fields is also studied.
