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TURKISH JOURNAL OF PHYSICS

Modelling of devices for optoelectronic applications: The quantum confined Stark effect and self-electrooptic effect devices

Eckehard Schöll

Published Dec 3, 1999• 3 citations
OpenAlex

Abstract

Electro-optical effects, such as the Franz-Keldysh effect in bulk materials or the quantum confined Stark effect in quantum well structures, lead to strong optoelectronic nonlinearities which form the basis for optical modulators and optically bistable devices. They result from a modification of the optical absorption properties by an applied electric field and are particularly pronounced in the case of low dimensional semiconductors. We review theoretical modelling and computer simulations of such optoelectronic devices in particular for ZnSe based quantum well structures, where excitonic features dominate even at room temperature. The field dependent absorption spectra are calculated by a many-body theory including the full electron-electron interaction. The transition from the quantum confined Stark effect, which is found for well widths smaller than the exciton Bohr diameter, to the Franz-Keldysh effect, which corresponds to the limit of wide wells, is studied. Optical bistability and switching is found in R-SEED and D-SEED configurations, and the optimization of the device performance is discussed.

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Electro-optical effects, such as the Franz-Keldysh effect in bulk materials or the quantum confined Stark effect in quantum well structures, lead to strong optoelectronic nonlinearities which form the basis for optical modulators and optically bistable devices. They result from a modification of the optical absorption properties by an applied electric field and are particularly pronounced in the case of low dimensional semiconductors. We review theoretical modelling and computer simulations of such optoelectronic devices in particular for ZnSe based quantum well structures, where excitonic features dominate even at room temperature. The field dependent absorption spectra are calculated by a many-body theory including the full electron-electron interaction. The transition from the quantum confined Stark effect, which is found for well widths smaller than the exciton Bohr diameter, to the Franz-Keldysh effect, which corresponds to the limit of wide wells, is studied. Optical bistability and switching is found in R-SEED and D-SEED configurations, and the optimization of the device performance is discussed.
We present computer simulations of self-electro-optic effect devices in different circuit environments, based on the quantum confined Stark effect in wide-gap materials with strong excitonic features. Our work is founded on a microscopic model of the electric field dependent absorption in ZnCdSe/ZnSSe quantum well structures, taking full account of Coulomb induced intersubband coupling and strong excitonic effects, which is essential for all wide-gap materials and distinguishes our theory from standard models of III–V compounds. Optical bistability and even multistability are predicted from the electro-optical and optical input–output characteristics for a wide range of operating conditions. The dependence upon the optical frequency, bias voltage, length of the waveguide and quantum well width, and possible optimization of the performance of the electro-optic modulator are discussed.
Abstract This paper briefly reviews the nonlinear optical and electro-optical properties and applications of GaAs—AlGaAs multiple quantum wells, all of which are compatible with laser diodes or semiconductor electronics or both. They show large nonlinear absorption and refraction (associated with their strong room-temperature exciton resonances) applicable to all-optical devices. They also show large electroabsorptive effects, some of which are unique to the quantum wells at any temperature, which are so strong that optical modulators can be made with micrometre dimensions. A new class of optical bistability (due to increasing absorption) is also reviewed; combination of this with the electroabsorptive effects enables a new mirrorless optical switch called a Self Electro-optic Effect Device (SEED), which sets a new standard for optical switching energies, with energy densities reduced by a factor of six by comparison to even the best resonant cavity devices.
The quantum confined Stark effect has found wide application in devices for optical modulation and bistable switching. Whilst normally-incident strained layer modulators and self electro-optic effect devices (SEEDs) have been demonstrated [1-3], the introduction of strain has provided little performance advantage. Recently there has been a growing interest in the properties of strained piezoelectric structures resulting from growth on orientations other than the (100) [4-6]. In this communication we present the results of an investigation of the electro-optical absorption modulation properties of a strained InGaAs/GaAs multiple quantum well p-i(MQW)-n grown on a (111)B GaAs substrate. Subsequently we demonstrate optical bistability using the self electro-optic effect without the application of an external bias.
The authors present a new type of optically bistable phase modulator utilizing a self electrooptic effect device (SEED) integrated with an electrooptic wavelength modulator. An electrically bistable SEED, operating on the principle of the quantum-confined Stark effect, controls the bias voltage across an electrooptic waveguide phase modulator to produce optical bistability. A control signal at 0.848 mu m, corresponding to the first electron to heavy hole exciton transition in GaAs/AlGaAs multiple-quantum-well is used to switch 1.152 mu m light propagating through a waveguide in a direction normal to the control beam.>
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.
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.