Abstract

Coherence effects arising due to Andreev reflections in a superconductor--insulator--normal-metal junction are considered. It is shown that in the absence of electron-electron interaction in the metal at low temperatures, the electrical potential drop on the insulator ${\mathit{I}}_{0}$${\mathit{R}}_{\mathit{I}}$, caused by the current density ${\mathit{I}}_{0}$ through the junction, vanishes, although the resistance of the device ${\mathit{R}}_{\mathrm{\ensuremath{\infty}}}$ measured by the two-probe method can be large. The electron-electron interaction determines the zero-temperature value of ${\mathit{R}}_{\mathit{I}}$. The implications of these effects for the theory of the superconductor--normal-metal--superconductor junction are discussed.

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