A photoconductive switch is an electrical switch which is based on the photoconductivity of a material, i.e. an increase in its electrical conductance as a consequence of irradiation with light. In nearly all cases, one uses a semiconductor material, where the absorbed light (with a photon energy above the bandgap energy) generates free carriers, which then contribute to the conductivity. Frequently used materials are chromium-doped gallium arsenide (Cr-GaAs), low-temperature grown gallium arsenide (LT-GaAs), indium phosphide (InP), amorphous silicon, and silicon on sapphire (SoS). In order to reduce the recovery time of the switch (determined by the lifetime of photoexcited carriers), one typically uses low-temperature growth (often followed by rapid thermal annealing), some doping (e.g. chromium in GaAs), or ion bombardment for producing crystal defects. Apart from the recovery time, important criteria are the bandgap energy, dark resistivity, and electrical breakdown resistance.
There are different designs of photoconductive switches:
- bulk devices several millimeters or even centimeters long with electrical contacts on the end faces, used for switching very high voltages (sometimes above 100 kV)
- devices with a small gap in a microstrip; the gap can be straight or interdigitated and has a width between a few microns and tens of microns; for low-power applications with very high speed
- sliding contact devices for the highest speed, where a point between the two parallel strips of a coplanar stripline is illuminated
All such devices are of the metal–semiconductor–metal (MSM) type.
Photoconductive switches are used for various purposes:
- for photoconductive sampling, particularly for testing of high-speed integrated electronic circuits (even before dicing the wafer, because electrical contacts are required only for DC and low-frequency signals)
- for the generation of terahertz pulses
- for the generation of microwaves and millimeter waves via direct DC to RF conversion, in both continuous-wave and pulsed mode (e.g. with a frozen waveform generator)
- as high-speed photodetectors in optical fiber communications
- in very fast analog-to-digital converters
|||F. W. Smith et al., “Picosecond GaAs-based photoconductive optoelectronic detectors”, Appl. Phys. Lett. 54 (10), 890 (1989)|
|||D. Krokel et al., “Subpicosecond electrical pulse generation using photoconductive switches with long carrier lifetimes”, Appl. Phys. Lett. 54, 1046 (1989)|
|||C. H. Lee, “Picosecond optics and microwave technology”, IEEE Trans. Microwave Theory Technol. 38 (5), 596 (1990)|
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