It is well known that a complex four-component Dirac spinor defines an
orthonormal tetrad on hat Minkowski spacetime, For example, a spinor
solution to the Dirac equation determines the four-velocity and Pauli-
Lubanski spin vector, comprising the timelike and first spacelike memb
ers of the particle's tetrad, as well as two other spacelike members t
hat are rarely discussed. Also, of particular note is the complex null
tetrad formalism that provides a map from a two-component SL (2, C) s
pinor and its complex conjugate to a tetrad. The inverse problem is st
udied here. Given a tetrad, a complex Dirac spinor valued function of
the tetrad is explicitly defined in such a way that certain sums of bi
linear products of the components of this spinor exactly reproduce the
tetrad. This spinor may be used in the Feynman propagator representat
ion of the solution to the Dirac equation to generate a Dirac wave spi
nor with desired initial properties. The mappings studied here represe
nt a new class of nonlinear mappings SO(3,2)(+)(1) --> SO(3,1). (C) 19
97 American Institute of Physics.