We present a description of spin-polarized transport in mesoscopic ferromagnet-superconductor $(F/S)$ systems, where the transport is diffusive and the interfaces are transparent. It is shown that the spin reversal associated with Andreev reflection generates an excess spin density close to the $F/S$ interface, which leads to a spin contact resistance. Expressions for the contact resistance are given for two-terminal and four-terminal geometries. In the latter the sign depends on the relative magnetization of the ferromagnetic electrodes.
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Jedema et al. (1999) studied this question.
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