  We construct the higher-spin massive fermionic fields in 2+1 dimensions.
Their field equations and propagators are derived from first principle. For
fields with j>1/2, complications arise from the non-linear behaviour of the
boost operators. We find that for a spin-three-half field, the non-linearity
have an underlying structure that guarantees the locality of the fields and the
existence of covariant propagators. We conjecture that this structure exists
for fields of all spin.
