The Rashba Hamiltonian describes the splitting of the conduction band as a
result of spin-orbit coupling in the presence of an external field and is c
ommonly used to model the electronic structure of confined narrow-gap semic
onductors. Due to the mixing of spin states some care has to be exercised i
n the calculation of transport properties. We derive the velocity operator
for the Rashba-split conduction band and demonstrate that the transmission
of an interface between a ferromagnet and a Rashba-split semiconductor does
not depend on the magnetization direction, in contrast with previous asser
tions in the literature.