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

机译:厚的0.35μmCMOS单光子雪崩二极管雪崩瞬变

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摘要

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.
机译:研究了两种具有不同直径的单光子雪崩二极管(SPAD)关于其雪崩行为。 SPAD型A在标准的0.35-μm互补金属氧化物 - 半导体(CMOS)中设计了包括12μm厚的P-EPI层,直径为50,100,200和400μm;并且B型在该过程的高压(HV)线中实现,直径为48.2和98.2μm。每个选隙都是引线连接到0.35-μm的CMOS时钟选通芯片,其在一个时钟周期期间控制充电到最大6.6V过量偏置,有效和淬火相以及读出。光子击中后的阴极电压的测量结果为50μm直径为4.2V和3.45ns的50-μm直径的50-μm直径偏置的下降时间(80%至20%)。对于4.26V的过量偏压,对于B型,48.2μm直径为8 ns的下降时间和5.4-V过量偏压以及98.2μm直径为5.9-μm和5.9V过量偏差。在通过连接的栅极芯片连接的示意图的阴极处的整体电容中,计算通过检测器的雪崩电流。这导致峰值雪崩电流,例如1.19 mA用于100μmspad型A和1.64 mA,用于98.2-μm型型B,分别为5和4.9 V的过量偏压。

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