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厚0.35微米CMOS单光子雪崩二极管的雪崩瞬变

Avalanche Transients of Thick 0.35 µm CMOS Single-Photon Avalanche Diodes.

作者信息

Goll Bernhard, Steindl Bernhard, Zimmermann Horst

机构信息

Institute of Electrodynamics, Microwave and Circuit Engineering, TU Wien, Gusshausstrasse 25/E354-02, A-1040 Wien, Austria.

出版信息

Micromachines (Basel). 2020 Sep 19;11(9):869. doi: 10.3390/mi11090869.

Abstract

Two types of single-photon avalanche diodes (SPADs) with different diameters are investigated regarding their avalanche behavior. SPAD type A was designed in standard 0.35-µm complementary metal-oxide-semiconductor (CMOS) including a 12-µm thick p epi-layer with diameters of 50, 100, 200, and 400 µm; and type B was implemented in the high-voltage (HV) line of this process with diameters of 48.2 and 98.2 µm. Each SPAD is wire-bonded to a 0.35-µm CMOS clocked gating chip, which controls charge up to a maximum 6.6-V excess bias, active, and quench phase as well as readout during one clock period. Measurements of the cathode voltage after photon hits at SPAD type A resulted in fall times (80 to 20%) of 10.2 ns for the 50-µm diameter SPAD for an excess bias of 4.2 V and 3.45 ns for the 200-µm diameter device for an excess bias of 4.26 V. For type B, fall times of 8 ns for 48.2-µm diameter and 5.4-V excess bias as well as 2 ns for 98.2-µm diameter and 5.9-V excess bias were determined. In measuring the whole capacitance at the cathode of the SPAD with gating chip connected, the avalanche currents through the detector were calculated. This resulted in peak avalanche currents of, e.g., 1.19 mA for the 100-µm SPAD type A and 1.64 mA for the 98.2-µm SPAD type B for an excess bias of 5 and 4.9 V, respectively.

摘要

研究了两种不同直径的单光子雪崩二极管(SPAD)的雪崩行为。A型SPAD采用标准的0.35μm互补金属氧化物半导体(CMOS)工艺设计,包括一个12μm厚的p外延层,直径分别为50、100、200和400μm;B型SPAD则在该工艺的高压(HV)线路中实现,直径分别为48.2和98.2μm。每个SPAD通过引线键合连接到一个0.35μm的CMOS时钟门控芯片,该芯片在一个时钟周期内控制高达6.6V的过偏置电荷、激活和猝灭阶段以及读出。对A型SPAD在光子撞击后的阴极电压进行测量,结果表明,对于直径为50μm的SPAD,在4.2V的过偏置下,下降时间(80%至20%)为10.2ns;对于直径为200μm的器件,在4.26V的过偏置下,下降时间为3.45ns。对于B型SPAD,直径为48.2μm且过偏置为5.4V时下降时间为8ns,直径为98.2μm且过偏置为5.9V时下降时间为2ns。在连接门控芯片的情况下测量SPAD阴极的总电容时,计算了通过探测器的雪崩电流。结果表明,对于A型100μm的SPAD,在5V的过偏置下,峰值雪崩电流为1.19mA;对于B型98.2μm的SPAD,在4.9V的过偏置下,峰值雪崩电流为1.64mA。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1668/7569859/f0660e2ae064/micromachines-11-00869-g001.jpg

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