Abstract
We formulate a microscopic theory of non-local electron transport in three-terminal diffusive normal-superconducting-normal (NSN) structures with arbitrary interface transmissions. At low energies we predict strong enhancement of non-local spectral conductance due to quantum interference of electrons in disordered N-terminals. In contrast, non-local resistance remains smooth at small and, furthermore, is found to depend neither on parameters of NS interfaces nor on those of N-terminals. At higher temperatures exhibits a peak caused by the trade-off between charge imbalance and Andreev reflection. Our results are in a good agreement with recent experimental observations and can be used for quantitative analysis of future experiments.
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