Anomalous transport in normal-superconducting and ferromagnetic-superconducting nanostructures

Abstract

We have calculated the temperature dependence of the conductance variation ($δS(T)$) of mesoscopic superconductor normal metal(S/N) structures, in the diffusive regime, analysing both weak and strong proximity effects. We show that in the case of a weak proximity effect there are two peaks in the dependence of $δS(T)$ on temperature. One of them (known from previous studies) corresponds to a temperature $T_1$ of order of the Thouless energy ($ε_{Th}$), and another, newly predicted maximum, occurs at a temperature $T_2$ where the energy gap in the superconductor $Δ(T_2)$ is of order $ε_{Th}$. In the limit $L_ϕ<L$ the temperature $T_1$ is determined by $D \hbar /L^2_ϕ$ ($L_ϕ$ is the phase breaking length), and not $ε_{Th}$. We have also calculated the voltage dependence $ δS(V)$ for a S/F structure (F is a ferromagnet) and predict non-monotonic behaviour at voltages of order the Zeeman splitting.