Abstract
The paper develops the theory of the field effect at high frequencies, using the same basic assumptions as Garrett (1957), with more complete conditions at the back surface. The charges induced in the front surface layer are given as the sums of two terms, of which one depends on the surface properties only, and the other is proportional to the modulation of the carrier density at the boundary between the surface layer and the bulk, which depends on the filament lifetime. The results are illustrated in detail by e numerical example.

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