Abstract

AbstractIn the nearly 45 years since Stan Ovshinsky's original publication [Phys. Rev. Lett. 21, 1450 (1968)] announcing the discovery of electric‐field‐induced threshold switching in chalcogenide alloy semiconductor glass thin films, the field of amorphous semiconductor physics has developed remarkably. Many commercial applications of these materials have been developed, including X‐ray image intensifiers, photocopier photoreceptors, and optical and electrical phase change memory devices. Despite these developments, a universally agreed upon, comprehensive model for the Ovshinsky Effect threshold switch still has not emerged. This paper is a brief review of the present state of understanding of this fascinating solid state physics phenomenon.

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