Andreev reflection in ferromagnet-superconductor junctions is derived in a
regime in which Zeeman splitting dominates the response of the superconduct
or to an applied magnetic field. Spin-up and spin-down Andreev reflections
are shown to be resolved as the voltage is increased. In the metallic limit
, the transition from Andreev to quasiparticle transport in the spin-up cha
nnels has a non-trivial behavior when spin polarization increases. The cond
uctance is asymmetric in a voltage reversal, which can be used as a new pro
be of spin polarization.