吸收倍增分离型雪崩器件的穿通现象研究
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北京工业大学

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国家自然科学基金项目(面上项目,重点项目,重大项目)(N0. 62375008);国家重点基础研究发展计划(973计划)(No. 2021FYB2206500);中科院青年基础研究项目 (No. YSBR-056);前沿科学重点研究计划 (ZDBS-LY-JSC008)


Research on the Punch-through Phenomenon of Separate Absorption, Charge, and Multiplication Avalanche Photodetectors
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Beijing University Of Technology

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The National Natural Science Foundation of China (N0. 62375008); National key Research and Development Program of China(No. 2021FYB2206500); CAS Project for Young Scientists in Basic Research (No. YSBR-056); Key Research Program of Frontier Sciences, CAS (ZDBS-LY-JSC008)

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    摘要:

    本文研究了吸收倍增分离型雪崩光电探测器(SACM APD)的穿通特性,基于器件的光谱响应、电容特性以及不同工作温度下的I-V特性,结合SILVACO仿真平台计算得到的器件内部电场和能带分布,分析了SACM APD穿通前后器件性能并建立相应的数学模型。设计优化硅基SACM APD器件结构参数和工艺参数,当场控层离子注入能量为580keV时,仿真得到,优化结构器件的穿通阈值电压为-30V,电容降低至穿通前的1/3。基于CMOS工艺制备了硅SACM APD器件,测试得到器件的穿通阈值电压为-30V,穿通时光电流升高至原来的2.18倍@808nm,响应峰值波长由穿通前的590nm红移至穿通后的820nm,峰值响应度由0.171A/W@590nm升高至0.377A/W@820nm,电容降低为穿通前的1/3@1MHz。

    Abstract:

    In this paper, the punch-through phenomenon was studied, based on a fabricated separate absorption, charge, and multiplication avalanche photodetector (SACM APD). The spectral response, capacitance characteristics, and I-V characteristics at different operating temperatures of the APD were measured and analyzed. Meanwhile, the device performance before and after the punch-through phenomenon were compared, and the model of the electric field region formed by external voltage was analyzed, based on the measurement results and the simulated the electric field and energy band distributions by the SILVACO. When the ion implantation energy of the charge layer was 580keV, the simulated device has a punch-through voltage of -30V and a capacitance reduction of one-third before punch-through. Then a Si SACM APD was prepared based on CMOS process. The punch-through voltage of the device was -30V and the capacitance was reduced to 1/3@1MHz before punch-through, which exactly match the simulation results. Moreover, the photocurrent after punch-through increases to 2.18 times of the before value at 808nm. The peak responsivity increases from 0.171A/W@590nm to 0.377A/W@820nm.

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  • 收稿日期:2024-09-10
  • 最后修改日期:2024-10-24
  • 录用日期:2024-10-29
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