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Electronics Letters

Nonbiased optical bistable device in an impedance-mismatchedasymmetric Fabry-Perot structure

Young‐Wan Choi, Oh Kee Kwon, Jongho Baek, B. Lee, E.-H. Lee

Published Nov 10, 1994• 9 citations
Publisher

Abstract

It is shown that nonbiased optical bistability in an extremely shallow quantum well symmetric self-electro-optic effect device can be significantly improved by using an impedance-mismatched asymmetric Fabry-Perot scheme. The device in a simple layout shows nonbiased bistability width, ΔR, contrast, and Vop of ~53%, 17%, 3.7:1, and 0.9 V, respectively.

DOI
10.1049/el:19941325

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It is shown that nonbiased optical bistability in an extremely shallow quantum well symmetric self-electro-optic effect device can be significantly improved by using an impedance-mismatched asymmetric Fabry-Perot scheme. The device in a simple layout shows nonbiased bistability width, ΔR, contrast, and Vop of ~53%, 17%, 3.7:1, and 0.9 V, respectively.
We have constructed a non-biased all-optical bistable device using electroabsorption in multiple quantum wells (MQWs). The device is made of a serial connection of two identical double p-i-n (p-i-n-i-p) diode structures within asymmetric Fabry–Perot (AFP) cavity. This scheme ensures both large internal electric field swing and full exploitation of the light intensity. From the measurement of the diode properties, the non-biased bistability parameters—reflection change of 19%, contrast ratio of 17:1, and bistable loop width of 70%—were obtained.
We demonstrated the optical bistable responses of the self-electro-optic effect device without applying any external bias. The function was realized by taking advantage of the significant electric-field dependence of both intensity and wavelength of an excitonic absorption peak, which is related to a resonance of electron levels in an asymmetric coupled quantum well structure. The successful result suggests that it is possible to create an all-optical bistable device with nonsegmented planar structure.
It is shown theoretically that optical bistability is possible in a self-electro-optic effect device (SEED) with single asymmetric quantum wells because of the blue shift of the optical absorption edge with applied field possible in such structures (in contrast to the normal red shift in symmetric wells). The concept is a simplification of the scheme of J. Khurgin [Appl. Phys. Lett. 53, 779 (1988)] (which uses unequal, opposed pairs of asymmetric wells) and shares the potential advantages of lower loss in the transmitting state and less stringent requirements on the exciton absorption peaks.