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Digest on Nonlinear Optics: Materials, Phenomena and Devices

Low Power Optical Switching In GaAs Epitaxial Etalons

J. L. Oudar, Bruno G. Sfez, Robert Kuszelewicz

Published Jan 1, 1990• 0 citations
Publisher

Abstract

Epitaxial methods allow the fabrication of nonlinear interferometric structures which include the mirrors and the nonlinear medium in a single crystal. Optical bistability is observed in these structures at mW optical power. The large excitonic and band-gap resonant nonlinearities of direct-gap semiconductors, such as bulk GaAs or Multiple Quantum Wells (MQW), allow to reach a substantial phase-shift (0.2-0.3 radian) over interaction lengths as small as a few wavelengths. This results in very compact nonlinear microcavities, with typically 5μm overall thickness.

DOI
10.1109/nlo.1990.695850

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Epitaxial methods allow the fabrication of nonlinear interferometric structures which include the mirrors and the nonlinear medium in a single crystal. Optical bistability is observed in these structures at mW optical power. The large excitonic and band-gap resonant nonlinearities of direct-gap semiconductors, such as bulk GaAs or Multiple Quantum Wells (MQW), allow to reach a substantial phase-shift (0.2-0.3 radian) over interaction lengths as small as a few wavelengths. This results in very compact nonlinear microcavities, with typically 5μm overall thickness.
Epitaxial methods allow the fabrication of nonlinear interferomethc structures which include the mirrors and the GaAs Multiple Quantum Wells (MQW) nonlinear medium in a single crystal. This results in very compact nonlinear microcavities with typically 5im overall thickness. Optical bistability is observed in these structures at mW optical power. We review our latest experimental results on these structures including the observation of high contrast switching in the reflection mode the direct measurement of dispersive optical nonlinearities in MQWs evidencing their saturation behavior at high intensities. Finally we report external-beam switching experiments which allow to assess the potential of these structures as all-optical gates.
Optical bistable devices containing GaAs/AlGaAs multiple quantum well (MQW) structures have shown great potential for performing fast low-power optical switching at room temperature.1 The presence of a much stronger exciton absorption feature in the MQW structures compared to bulk GaAs suggests far superior performance in the former. We report the observation of room-temperature bistability in bulk GaAs with input power <10 mW and intensities of a few kW/cm2. The intensities are consistent with the data of Miller et al.2 which show a saturation intensity of nearly 4 kW/cm2 in a MQW sample with a detuning of less than a halfwidth from the peak of the exciton resonance. Our detunings are always several halfwidths.
Abstract An experimental study is made of GaAs/AlGaAs monolithic bistable etalons fabricated by metalorganic vapor‐phase epitaxy. Optical bistability is observed in the reflective mode, with a minimum threshold power of less than 3 mW and a switching contrast as high as 30: 1, with a cavity resonator designed to achieve simultaneously a high finesse and a high reflectivity contrast. The dispersive optical nonlinearity of the multiple quantum well active medium is measured as a function of the intracavity intensity, and a strong saturation behavior is observed. The origin of this saturation and its implication on the design of future devices is discussed briefly.
Semiconductors exhibit large optical nonlinearities near the band edge because of resonance enhancement. Optical bistability occurs when the optical nonlinearities are coupled with feedback. In bulk GaAs and GaAs–AlGaAs multiple-quantum-well superlattices, the nonlinearity arising from the presence of the free-exciton resonance has produced room-temperature optical bistability with a few milliwatts of power. The formation of biexcitons in CuCl, the saturation of the bound exciton on CdS, and band-filling effects in InSb, InAs, and HgCdTe lead to observation of bistability in these materials. A bistable etalon can be operated in an optical-gate mode to generate optical analogs of electronic gates such as and, or, and nor. It has been demonstrated that a GaAs optical NOR gate responds in ∼1 psec, using only ≲3 pJ of energy. However, because of the carrier lifetime of a few nanoseconds, the repetition rate of the NOR gate is now limited to a few hundred megahertz.