The propagation of scalar and spinor fields in a spacetime whose metri
c changes signature is analyzed. The recent work of Dray, Manogue, and
Tucker on particle production from signature change for a (massless)
scalar field is reviewed, and an attempt is made to extend their analy
sis to the case of a (massless) spin-1/2 field. In contrast with their
results for a scalar field, it is shown here, for SL(2,C) spinors, th
at although there are inequivalent forms of the Dirac equation that ca
n be used to propagate a spinor in a signature-changing spacetime, non
e of these forms gives rise to a conserved inner product on the space
of solutions to the field equations.