metal–semiconductor–metal photodetectors (original) (raw)
Acronym: MSM photodetector
Definition: fast photodetector devices based on metal–semiconductor (Schottky) contacts
- photodetectors
- infrared detectors
- position-sensitive detectors
- photodiodes
- phototransistors
- metal–semiconductor–metal photodetectors
- velocity-matched photodetectors
- photomultipliers
- phototubes
- pyroelectric detectors
- photoconductive detectors
- photoemissive detectors
- solar-blind photodetectors
- single-photon detectors
- terahertz detectors
- velocity-matched photodetectors
- (more topics)
Related: photodetectorsphotodiodesbandwidth
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DOI: 10.61835/gio Cite the article: BibTex BibLaTex plain textHTML Link to this page! LinkedIn
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A metal–semiconductor–metal photodetector (MSM detector) is a photodetector device containing two Schottky contacts, i.e., two metallic electrodes on a semiconductor material, in contrast to a p–n junction as in a photodiode. It is thus a kind of Schottky barrier detector, but with two Schottky junctions. During operation, some electric voltage is applied to the electrodes. When light impinges on the semiconductor between the electrodes, it generates electric carriers (electrons and holes), which are collected by the electric field and thus can form a photocurrent.
One normally uses some kind of interdigitated electrode structure, where the finger spacing can be as small as 1 μm. The electrode structure can also be ring-shaped, covering an approximately circular area. Light hitting the device from the side of the electrodes is partially blocked by the electrodes, which of course reduces the quantum efficiency — unless the light is fully directed to the area between electrodes. For higher quantum efficiencies, there are back-illuminated devices, where the light impinges from the other side, so that it is not hindered by the electrodes. Another possibility is to use top illumination in combination with extremely thin gold contacts, which are partially transparent. An advantage of top illumination is that the achieved detection bandwidth is usually higher, since the carriers are generated closer to the contacts.
For highest speeds, traveling-wave configurations are used, where the input light is sent through an optical waveguide containing the absorbing layer. The electrodes are deposited on top of the waveguide, forming a coplanar waveguide line for the generated microwave signal.
MSM detectors can be made faster than photodiodes. Their detection bandwidths can reach hundreds of gigahertz (with an impulse response function narrower than 1 ps), making them suitable for very high-speed optical fiber communications.
A practically important aspect is that MSM photodetectors, having a relatively simple planar structure, are particularly suitable for monolithic integration with other components on photonic integrated circuits.
Frequently Asked Questions
This FAQ section was generated with AI based on the article content and has been reviewed by the article’s author (RP).
What is a metal-semiconductor-metal (MSM) photodetector?
An MSM photodetector is a device featuring two metallic electrodes that form Schottky contacts on a semiconductor material. Unlike a conventional photodiode, it does not rely on a p–n junction.
How does an MSM photodetector work?
When light illuminates the semiconductor material between the electrodes, it generates electric carriers (electrons and holes). An applied voltage creates an electric field that collects these carriers, resulting in a measurable photocurrent.
What are the main advantages of MSM photodetectors?
MSM photodetectors can achieve higher speeds than photodiodes, with detection bandwidths of hundreds of gigahertz. Their simple planar structure makes them particularly well-suited for monolithic integration into photonic integrated circuits.
How can the quantum efficiency of MSM photodetectors be improved?
To prevent the metal electrodes from blocking incident light, MSM detectors can be back-illuminated, so light enters from the substrate side. Another method is to use top illumination with extremely thin, partially transparent metal electrodes.
Bibliography
| [1] | W. C. Koscielniak et al., “Dynamic behavior of photocarriers in a GaAs metal–semiconductor–metal photodetector with sub-half-micron electrode pattern”, Appl. Phys. Lett. 54 (6), 567 (1989); doi:10.1063/1.100933 |
|---|---|
| [2] | J. B. D. Soole and H. Schumacher, “InGaAs metal–semiconductor–metal photodetectors for long wavelength optical communications”, IEEE J. Quantum Electron. 27 (3), 737 (1991); doi:10.1109/3.81384 |
| [3] | C. Moglestue et al., “Picosecond pulse response characteristics of GaAs metal–semiconductor–metal photodetectors”, J. Appl. Phys. 70 (4), 2435 (1991); doi:10.1063/1.349395 |
| [4] | S. Y. Chou et al., “Ultrafast nanoscale metal–semiconductor–metal photodetectors on bulk and low-temperature grown GaAs”, Appl. Phys. Lett. 61 (7), 819 (1992); doi:10.1063/1.107755 |
| [5] | J.-W. Shi et al., “metal–semiconductor–metal traveling-wave photodetectors”, IEEE Photon. Technol. Lett. 13 (6), 623 (2001); doi:10.1109/LEOS.2002.1159372 |
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