We study the subgap conductance of a ferromagnetic mesoscopic region attached to a ferromagnetic and a superconducting electrode by means of tunnel junctions. In the absence of the exchange field, the ratio r=γ/εT of the two-tunnel junction resistances determines the behavior of the subgap conductance, which possesses a zero-bias peak for r1 and for r1 a peak at finite voltage. We show that the inclusion of the exchange field leads to a peak splitting for r1, while it shifts the zero-bias anomaly to finite voltages for r1.
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Leadbeater et al. (1999) studied this question.
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