彭超, 周杨, 陈中圆, 雷志锋, 马腾, 张战刚, 张鸿, 何玉娟. 直流输电用特高压晶闸管大气中子失效率评估和损伤机理[J]. 原子能科学技术, 2024, 58(1): 248-256. DOI: 10.7538/yzk.2023.youxian.0092
引用本文: 彭超, 周杨, 陈中圆, 雷志锋, 马腾, 张战刚, 张鸿, 何玉娟. 直流输电用特高压晶闸管大气中子失效率评估和损伤机理[J]. 原子能科学技术, 2024, 58(1): 248-256. DOI: 10.7538/yzk.2023.youxian.0092
PENG Chao, ZHOU Yang, CHEN Zhongyuan, LEI Zhifeng, MA Teng, ZHANG Zhangang, ZHANG Hong, HE Yujuan. Evaluation of Atmospheric Neutron Failure Rates and Damage Mechanisms of Ultra-high Voltage Thyristor for DC Transmission[J]. Atomic Energy Science and Technology, 2024, 58(1): 248-256. DOI: 10.7538/yzk.2023.youxian.0092
Citation: PENG Chao, ZHOU Yang, CHEN Zhongyuan, LEI Zhifeng, MA Teng, ZHANG Zhangang, ZHANG Hong, HE Yujuan. Evaluation of Atmospheric Neutron Failure Rates and Damage Mechanisms of Ultra-high Voltage Thyristor for DC Transmission[J]. Atomic Energy Science and Technology, 2024, 58(1): 248-256. DOI: 10.7538/yzk.2023.youxian.0092

直流输电用特高压晶闸管大气中子失效率评估和损伤机理

Evaluation of Atmospheric Neutron Failure Rates and Damage Mechanisms of Ultra-high Voltage Thyristor for DC Transmission

  • 摘要: 本文基于散裂中子源开展了直流输电用8.5 kV/5 kA晶闸管的加速辐照试验。试验证实了大气中子导致的晶闸管单粒子烧毁失效现象,同时基于加速辐照试验结果计算了大气中子导致的晶闸管失效率。晶闸管的反向偏置电压和结温是影响晶闸管器件失效的关键因素。大气中子失效率随着反向偏置电压的增加呈指数增加。此外,失效率随温度的降低而增加。对应器件偏置在50%额定电压下的情况,5 ℃时的失效率较25 ℃时增加了近6倍。基于TCAD仿真进一步验证了辐照导致晶闸管失效的机理。仿真表明,单粒子烧毁失效与辐射粒子入射诱发的雪崩击穿效应直接相关。雪崩击穿效应与晶闸管反向偏置电压正相关,而与结温负相关,这与大气中子失效率随电压和结温的变化关系一致。

     

    Abstract: As the core of high-voltage direct-current transmission technology, the DC converter valve and its key power device thyristor face a high risk of failure caused by atmospheric neutron when operating in high-altitude areas. The atmospheric neutron failure rate of thyristors used at high altitudes can be quantitatively evaluated by conducting accelerated irradiation tests. The accelerated irradiation experiments of 8.5 kV/5 kA thyristor for DC transmission were carried out at different temperatures by using the China spallation neutron source. The atmospheric neutron-induced single-event burnout (SEB) for thyristor was verified by experiments. It is manifested as a sudden surge in reverse bias leakage current during irradiation, and the device loses its high voltage blocking ability. The failure rates of thyristor caused by atmospheric neutrons were also evaluated based on the accelerated irradiation experimental results. The reverse bias voltages and junction temperatures of thyristor are the key factors affecting the failure rates. The atmospheric neutron-induced failure rates increase exponentially with the reverse bias voltage. The atmospheric neutron failure rate of the 8 500 V thyristor operating at 4 350 V will reach 673 FIT at room temperature at sea level; when the bias voltage drops to 4 100 V (a decrease of about 5.7%), the atmospheric neutron failure rate can be reduced to 11 FIT. In addition, the failure rate increases with the decrease of temperature. The failure rate at 5℃ is nearly 6 times higher than that at 25℃ when the device is biased at 50% of the rated voltage. Based on TCAD simulations, the failure mechanism of thyristor caused by irradiation is further verified. The simulation results show that the SEB failure is directly related to the avalanche breakdown effect-induced by the incident radiation particles. For radiation-induced SEB failure of thyristors, the sensitive region is the N-drift/P-substrate junction depletion region (corresponding to the electric field concentration region under reverse bias of thyristors). When radiation particles are incident into the sensitive region, it can cause the concentration of electric field near the incident location, resulting in additional electric field spikes. If the peak of the electric field exceeds the critical electric field Ec (about 1.64×105 V/cm), it will induce avalanche breakdown. The high voltage reverse bias high current state caused by avalanche breakdown ultimately leads to the failure of the thyristor. The avalanche breakdown effect is positively correlated with the reverse bias voltage of thyristor and negatively correlated with the junction temperature. This is consistent with the variation of atmospheric neutron failure rates with bias voltages and junction temperatures.

     

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