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Damage effect and mechanism of Darlington tubes caused by intense electromagnetic interference

Wang Qiankun Chai Changchun Xi Xiaowen Yang Yintang

王乾坤, 柴常春, 席晓文, 等. 强电磁干扰对达林顿管的损伤效应与机理[J]. 强激光与粒子束, 2018, 30: 083008. doi: 10.11884/HPLPB201830.170472
引用本文: 王乾坤, 柴常春, 席晓文, 等. 强电磁干扰对达林顿管的损伤效应与机理[J]. 强激光与粒子束, 2018, 30: 083008. doi: 10.11884/HPLPB201830.170472
Wang Qiankun, Chai Changchun, Xi Xiaowen, et al. Damage effect and mechanism of Darlington tubes caused by intense electromagnetic interference[J]. High Power Laser and Particle Beams, 2018, 30: 083008. doi: 10.11884/HPLPB201830.170472
Citation: Wang Qiankun, Chai Changchun, Xi Xiaowen, et al. Damage effect and mechanism of Darlington tubes caused by intense electromagnetic interference[J]. High Power Laser and Particle Beams, 2018, 30: 083008. doi: 10.11884/HPLPB201830.170472

强电磁干扰对达林顿管的损伤效应与机理

doi: 10.11884/HPLPB201830.170472
基金项目: 

the Open Fund of Key Laboratory of Complex Electromagnetic Environment Science and Technology, China Academy of Engineering Physics 2015-0214.XY.K

详细信息
  • 中图分类号: TN322.8

Damage effect and mechanism of Darlington tubes caused by intense electromagnetic interference

Funds: 

the Open Fund of Key Laboratory of Complex Electromagnetic Environment Science and Technology, China Academy of Engineering Physics 2015-0214.XY.K

More Information
    Author Bio:

    Wang Qiankun(1990—), male, Master degree candidate, engaged in research of semiconductor devices and circuit reliability; wang__qk@163.com

  • 摘要: 建立了PNP型达林顿管的二维电热模型,对处于有源放大区的达林顿管的集电极注入高功率微波(HPM)和强电磁脉冲(EMP)时的瞬态响应进行了仿真。结果表明:HPM注入下,器件内部的峰值温度呈周期性的“下降-上升”,温度升高过程发生在信号的正半周,靠近达林顿管发射极的晶体管发射结边缘是最易毁伤处;EMP注入下,其损伤机理与HPM注入时的正半周时相似,器件内部峰值温度一直上升,易毁伤部位与HPM注入时相同。得到了损伤功率阈值和损伤能量阈值与损伤脉宽的关系,这两种干扰注入下的损伤能量阈值-脉宽关系和损伤功率阈值-脉宽关系公式相似,并且在相同脉宽下,HPM注入下的损伤能量阈值大于EMP注入下的损伤能量阈值。
  • Figure  1.  Circuit schematic and device structure of PNP type Darlington tube

    Figure  2.  Simulation circuit diagram of Darlington tube

    Figure  3.  Variation of the maximum temperature within device with time

    Figure  4.  Distribution of (a) electric field, (b) current density and (c) temperature at 3.15 ns

    Figure  5.  Distribution of (a) electric field, (b) current density and (c) temperature at 3.75 ns

    Figure  6.  Variation of the maximum temperature within the Darlington tube with time

    Figure  7.  Distribution of (a) electric field, (b) current density and (c) temperature at burn-out time

    Figure  8.  Energy threshold and power threshold vs pulse width of EMP

    Figure  9.  Energy threshold and power threshold vs pulse width of HPM

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出版历程
  • 收稿日期:  2017-11-19
  • 修回日期:  2018-04-26
  • 刊出日期:  2018-08-15

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