Abstract
The author's older theory of conduction in polarizable media is generalized in such a way as to include rectification. An electronic component (positive holes or electrons) and an ionic component (negative or positive ions) are taken into account. The former are subjected to the boundary conditions of the MottSchottky theory, the latter to the boundary conditions of the author's theory of polarization. Significant deviations from the Mott-Schottky theory are caused by the ionic component.

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