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Philosophical Transactions of the Royal Society of London Series A Mathematical and Physical Sciences

Semiconductor nonlinear etalons

H. M. Gibbs, Jack L. Jewell, Nasser N. Peyghambarian, Michael C. Rushford, Kuochou Tai, S. S. Tarng, Doreen A. Weinberger, Arthur C. Gossard, W. Wiegmann, Thirumalai Venkatesan

Published Dec 18, 1984• 8 citations
Publisher

Abstract

Abstract Previous observations of optical bistability in nonlinear etalons of ZnS, CuCl and GaAs are summarized. Emphasis is placed upon recent results in GaAs: similar room-temperature optical bistability at powers under 10 mW in bulk and multiple quantum-well etalons; room-temperature bistability achieved with a diode laser as a light source; NOR and other logic operations; optical fibre signal regeneration and continuous wave operation.

DOI
10.1098/rsta.1984.0102

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Abstract Previous observations of optical bistability in nonlinear etalons of ZnS, CuCl and GaAs are summarized. Emphasis is placed upon recent results in GaAs: similar room-temperature optical bistability at powers under 10 mW in bulk and multiple quantum-well etalons; room-temperature bistability achieved with a diode laser as a light source; NOR and other logic operations; optical fibre signal regeneration and continuous wave operation.
Optical bistable devices may someday be the key elements of all-optical logic and computing systems.1 Semiconductor devices appear particularly promising because of very large optical nonlinearities permitting the construction of very small devices. The goal is to develop small (≃ 1 μm), fast (≃ 1 ps), low-power (≃ 1 μW), high-temperature (≃ 300 K) devices. Herein is reported room-temperature operation of GaAs devices that are similar in size, speed, and power to the low-temperature pure-GaAs device.2
In this paper we present the basic principles of optical bistability and summarize the current advances in semiconductor optical switching, with emphasis on recent results in GaAs, CuCI, InAs, InSb, CdS, ZnS, and ZnSe etalons. These devices have great potential for applications involving optical signal processing and computing. As an example, we discuss the use of arrays of bistable devices for parallel optical processing and for addressable spatial light modulators. The use of nonlinear etalons as optical gates is also illustrated. To date, GaAs devices have shown the most favorable characteristics for practical applications. They operate at room temperature with a few milliwatts of power using a laser diode as the only light source. Quasi-cw operation and optical fiber signal regeneration have also been demonstrated. A GaAs NOR gate operates in 1 ps with <3 pJ incident energy; this, of course, implies a 1 ps switch-on time for a bistable etalon.
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.
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.