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CRC Press eBooks

Nonlinear Optical Switching Devices

Wallace B. Leigh

Published May 12, 2021• 0 citations
Publisher

Abstract

An optical switching device may be defined as one that either diverts an optical beam from its path or that may be used as a source for optical modulation. An optical modulator would be used to modulate an optical signal, for example, to encode a digital signal onto a light beam. An optical switching device may be fabricated as a discrete component or incorporated into an optical waveguide. It must, ideally, consume low power and be operable at a comparatively low optical power level and high bandwidth. An optical switching device may be fabricated as a discrete component or incorporated into an optical waveguide. It must, ideally, consume low power and be operable at a comparatively low optical power level and high bandwidth. An ideal material for practical optical bistable applications is one which has a large nonlinearity and a relatively low absorption at the wavelength of interest, as this is the optimum condition for dispersive effects.

DOI
10.1201/9781003210283-6

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An optical switching device may be defined as one that either diverts an optical beam from its path or that may be used as a source for optical modulation. An optical modulator would be used to modulate an optical signal, for example, to encode a digital signal onto a light beam. An optical switching device may be fabricated as a discrete component or incorporated into an optical waveguide. It must, ideally, consume low power and be operable at a comparatively low optical power level and high bandwidth. An optical switching device may be fabricated as a discrete component or incorporated into an optical waveguide. It must, ideally, consume low power and be operable at a comparatively low optical power level and high bandwidth. An ideal material for practical optical bistable applications is one which has a large nonlinearity and a relatively low absorption at the wavelength of interest, as this is the optimum condition for dispersive effects.
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.
We present a review of optical bistability in active and passive optoelectronic devices, with particular reference to switching speeds and powers. The large resonant nonlinearities available near the bandgaps of semiconductors may be utilized to develop bistable devices operating at low powers and high speeds. Passive devices are driven by external optical sources and include nonlinear etalons, nonlinear interfaces, self-focusing configurations and electro-optic modulators with electrical feedback. Active devices include injection lasers and superluminescent amplifiers. Potential advantages of active devices include speed, gain, sensitivity and the ability to drive other devices, but complexity and high power dissipation may limit their use in applications requiring high density.
Optical bistable devices [1] are being developed with a view to their use as logic gates in optical processors [2]. The response of an optical bistable device is strongly nonlinear and once a device has been fabricated, its behaviour as a logic gate can still be modified to a large extent by the variation of certain parameters used to bias the device, Important responses include the device’s fanout potential, its switching speed and the contrast between its high and low output levels. Because of the complexity of the behaviour, it can be difficult to see how one response varies as another is improved. The method of ‘operating curves’ explained here allows a system designer to see how optimum performance may be attained.
This paper presents properties of all-optical bistable fibre switch using two fibre Bragg gratings and rare earth elements doped optical fiber. It is not possible to obtain bistable properties at low switching power level in case of a single fibre grating. In this article the method of optical switching that uses all-optical switch has been proposed. It has been achieved by varying the refractive index of nonlinear optical material as a result of light signal amplitude changes. Presented optical bistable device can be used both in contemporary optically switched networks as well as in optoelectronic sensors, owing to their high achievable resolution.
Bistable optical systems are of considerable interest to produce high-speed optical signal-processing devices. Among them, those that use a nonlinear optical medium are attractive because they allow the lowest possible switching time. By the use of a suitable electromagnetic resonance, the bistability threshold can be lowered to a reasonnable value, for the incident power. Keeping in mind that a bistable optical system should be well adapted to optical integration in a planar geometry, one is naturally confronted to a corrugated waveguide filled with a nonlinear (Kerr) medium.