  A covariant set of linear differential field equations, describing an N=1
supersymmetric anyon system in (2+1)D, is proposed in terms of Wigner's
deformation of the bosonic Heisenberg algebra. The non-relativistic
``Jackiw-Nair'' limit extracts the ordinary bosonic and fermionic degrees of
freedom from the Heisenberg-Wigner algebra. It yields first-order,
non-relativistic wave equations for a spinning particle on the non-commutative
plane that admits a Galilean exotic planar N=1 supersymmetry.
