Avalanche photodiode with uniform avalanche multiplication

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357 19, 357 13, 357 16, 357 61, 357 90, H01L 2714

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049357956

ABSTRACT:
An APD of the invention has its avalanche multiplication layer, made of a material which can cause a resonant impact ionization therein, between its window layer having a big band gap energy and light-absorbing layer having a band gap energy smaller than the window layer. The layout of the invention lowers field intensity in the light absorbing layer, thus, a dark current produced by a tunnel effect in the light absorbing layer is reduced. Because of great amount of ionization ratio in the resonant impact ionization phenomena, both excessive noise factor and the applied operating DC voltage to the APD can be much less than that of the prior art APD without employing the resonant impact ionization, as well as the operation speed can be increased. The reduced operation voltage protects unexpected local avalanche breakdown in the pn junction area, thus uniform and reliable avalanche multiplication is always initiated in the multiplication layer, resulting in reduction of dark current and allowing a voltage margin. For fabricating the APD, there is no difficult problem like the difficulty of doping n.sup.+ impurity in the p-type window layer in the prior art APD employing the resonant impact ionization. Excessive noise factor below 3, operation at 12.5 V, and operation at 10 GHZ are achieved.

REFERENCES:
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Anoo et al., "In GaAs/InP Separated Absorption and Multiplication Regions Avalanche Photodiode Using Liquid-and VaBr-Phase Epitaxies", IEEE Journal of Quantum Electronics, vol. QE-17, Feb., 1981, No. 2, New York, U.S.A., pp. 250-254.
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ECOC 83. 9th European Conference on Optical Communication, Geneva, Oct. 23-26, 1983, pp. 479-482, Elsevier Science Publishers B.V., "1.3mum CdHgTe Avalanche Photodiodes for Fiber Optic Applications", by G. Pichard et al.

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