Abstract

Silicon avalanche photodetector (APD) plays a very important role in near-infrared light detection due to its linear controllable gain and attractive manufacturing cost. In this paper, a silicon APD with punch-through structure is designed and fabricated by standard 0.5 μm complementary metal oxide semiconductor (CMOS) technology. The proposed structure eliminates the requirements for wafer-thinning and the double-side metallization process by most commercial Si APD products. The fabricated device shows very low level dark current of several tens Picoamperes and ultra-high multiplication gain of ~4600 at near-infrared wavelength. The ultra-low extracted temperature coefficient of the breakdown voltage is 0.077 V/K. The high performance provides a promising solution for near-infrared weak light detection.

Highlights

  • The following requirements for avalanche photodetector (APD) should be satisfied to enable the capability of weak light detection in light detection and ranging (LiDAR) systems [4]

  • The electrical field inside photons absorbing region and carrier multiplication region is controlled by the doping profile of the charge layer, which is the key to the Si APD design

  • Limited by the existing test equipment, the spectral response, the response speed, and the multiplication noise are not able to be presented in this paper

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Summary

Introduction

Avalanche photodetectors (APDs) have been widely used for weak light detection due to their large internal avalanche gain. Ge/Si APD [2,12] and APDs based on III-V semiconductor materials [13,14] with ultralow temperature dependency of the breakdown voltage have been demonstrated. These APDs have much higher multiplication excess noise than that of Si APDs due to the lower k-value (the ratio of ionization coefficient of holes over electrons) of silicon. A high-performance Si APD with lower temperature coefficient of 0.32 V/K was demonstrated [8], the wafer thinning process and the double-sided metallization required by such devices are not available for.

Device Design and Fabrication
Dark Current and Photocurrent
Terminal Capacitance
Responsivity and Gain
Conclusions
Full Text
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