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光控多门极晶闸管的多种工作模式

王凌云 刘宏伟 袁建强 谢卫平 栾崇彪 李洪涛 张建德 谌怡 何泱 刘小俐 高彬

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光控多门极晶闸管的多种工作模式

王凌云, 刘宏伟, 袁建强, 谢卫平, 栾崇彪, 李洪涛, 张建德, 谌怡, 何泱, 刘小俐, 高彬

Various operating modes of optically controlled multi-gate thyristors

WANG Lingyun, LIU Hongwei, YUAN Jianqiang, XIE Weiping, LUAN Chongbiao, LI Hongtao, ZHANG Jiande, CHEN Yi, HE Yang, LIU Xiaoli, GAO Bin
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  • 为了提升半导体开关的峰值功率与导通速度, 针对光控多门极晶闸管结构开展了系列实验研究, 重点探讨了不同光注入参数对开关特性的影响. 研究发现, 在不同激光峰值功率条件下, 开关芯片展现出不同的导通特性. 通过建立开关模型, 并对注入光参数及电路参数进行对比分析, 本工作提出了光控多门极晶闸管的3种工作模式设想: 光致线性模式(A模式)、场致非线性模式(C模式)和混合放大模式(B模式). 为验证这些工作模式, 我们进行了针对性的验证测试, 结果证实了该光控多门极晶闸管具有不同导通特性的工作模式. 开关多工作模式的发现与验证, 大幅度提升了功率半导体开关器件的斜率(di/dt)水平和峰值功率. 在23 mm直径芯片上, A模式获得了4 kV, 8 kA, 440 kA/μs的窄脉冲; C模式获得了8.5 kV, 6.0 kA, 55 kA/μs的宽脉冲; 在38 mm直径芯片上, B模式获得了4.6 kV, 8.5 kA, 129 kA/μs的宽脉冲. 这些成果为超高峰值功率半导体开关组件的研发奠定了坚实的理论与实验基础.
    In order to meet the switching requirements of high-frequency pulsed-power systems and further enhance the peak power and turn-on speed of solid-state switches, comparative experiments on the structure of optically controlled multi-gate thyristors and the parameter of injected light are investigated in this work. The research results show that semiconductor chips based on the multi-gate thyristor structure exhibit different conduction characteristics under varying laser injection conditions, resulting in unique inflection point curves. By establishing a switching model and changing the injected light parameters and circuit parameter models, three conceptual operating modes for the optically controlled multi-gate thyristor are proposed, they being photonic linear mode (Mode A), field-induced nonlinear mode (Mode C), and hybrid amplification mode (Mode B).Based on these concepts, the experimental validation tests are conducted, and the three distinct operating characteristics of the optically controlled multi-gate thyristor are confirmed. In Mode A, the conduction process is mainly related to the injected light power parameters, which is similar to the scenario in the linear mode of traditional light-guided switches, thus Mode A is suitable for the narrow pulse width applications. Mode C mainly focuses on carrier multiplication after injection, resembling the conduction characteristics of super thyristors (SGTO), and this mode is suitable for wide pulse width and high current applications. In Mode B, its initial conduction is related to the injected light parameters, while the later carrier multiplication continues from the earlier photonic linear mode, achieving characteristics of both fast rise time and wide pulse width, effectively integrating the advantages of light-guided switches and SGTOs.In Mode A, when injected laser energy is 8.5 mJ, a pulse width is 10 ns, and peak power is 0.85 MW, the switch operates at a voltage of 5.2 kV, an output current of 8.1 kA, turn-on time (10%—90%) of 18.4 ns, with a di/dt value reaching 440 kA/μs. The main characteristic is that the di/dt of the switch is linearly related to the injected laser energy, thereby achieving a fast rise time output, which reflects the photonic linear conduction mode. This mode is suitable for high-power, narrow-pulse, and fast-rise-time applications, such as high-power microwave sources, and its characteristics are similar to those of gas switches.In Mode C, when triggering laser energy is set to 250 μJ, a pulse width is 210 ns, and peak power is 1200 W, the switch operates at a voltage of 8.5 kV, a short-circuit current of 6 kA and a current rise time of 110 ns, achieving a di/dt value exceeding 55 kA/μs. The key characteristic is that the di/dt of the switch is unrelated to the injected laser energy but is related to the electric field applied across the switch, thus it can operates at large current and wide pulse width, which reflects the field-induced nonlinear conduction mode. This mode is suitable for high-power, wide-pulse, and slower-rise-time applications, such as large current detonation and electromagnetic drives, and its characteristics are similar to those of igniter tubes and triggered light.In Mode B, when triggering laser energy is set to 10 mJ, a pulse width is 20 ns, and peak power is 0.5 MW, the switch operates at a voltage of 4.6 kV, with a short-circuit current reaching 8.5 kA and a current rise time of 66 ns, achieving a di/dt value exceeding 129 kA/μs. The main characteristic is that the initial conduction of the switch satisfies the photonic linear conduction mode, while the later conduction exhibits the field-induced nonlinear conduction mode, thus achieving both fast-rise-time output and the capability for large current and wide pulse width, reflecting a hybrid conduction mode. This mode is suitable for high-power and wide-pulse applications, such as accelerator power supplies, its characteristics are similar to those of hydrogen thyratrons and pseudo-spark switches.The discovery and validation of multiple operating modes for the switch significantly enhance the di/dt and peak power of power semiconductor switching devices, laying a theoretical and experimental foundation for the development of semiconductor switches with ultra-high peak power. Additionally, the switching devices are packaged according to their different operating modes and have been used in accelerator power supplies, solid-state detonators, and high-stability pulse drive sources, achieving positive results.
  • 图 1  耐受直流型固态开关器件

    Fig. 1.  Direct current tolerant solid-state switching.

    图 2  脉冲或关断型固态开关器件

    Fig. 2.  Pulse or turn-off type solid-state switch.

    图 3  开关芯片结构示意图

    Fig. 3.  Schematic diagram of switch chip structure.

    图 4  器件元胞结构尺寸与正向电场分布图

    Fig. 4.  Cell structure dimensions and forward electric field distribution diagram of the chip.

    图 5  流片实现的多种尺寸的开关芯片

    Fig. 5.  Fabricated switch chips in various sizes.

    图 6  光控多门极晶闸管测试电路及照片 (a)测试电路原理图; (b)测试电路照片

    Fig. 6.  Optically controlled multi-gate thyristor test circuit and photos: (a) Schematic diagram of the test circuit; (b) photo of the test circuit.

    图 7  触发激光峰值功率与开关di/dt、导通延迟时间的关系图

    Fig. 7.  Graph of the relationship between trigger laser peak power and switch di/dt, turn-on delay time.

    图 8  注入激光峰值功率与开关输出峰值功率比值关系图

    Fig. 8.  Graph of the ratio relationship between injected laser peak power and switch output peak power.

    图 9  多种工作模式的设想及典型特征

    Fig. 9.  Conceptual designs and typical characteristic diagrams of various operating modes.

    图 10  电路仿真的光控多门极晶闸管电流电压曲线图

    Fig. 10.  Simulated current-voltage curve of an optically controlled multi-gate thyristor.

    图 11  电路中光控多门极晶闸管在0, 10, 70 ns时电子浓度分布

    Fig. 11.  Electron concentration distribution in the optically controlled multi-gate thyristor at 0, 10, and 70 ns in the circuit.

    图 12  电路仿真的光控多门极晶闸管电流电压曲线图

    Fig. 12.  Simulated current voltage curve diagram of an optically controlled multi-gate thyristor.

    图 13  电路中光控多门极晶闸管在0, 80, 600 ns时电子浓度分布图

    Fig. 13.  Electron concentration distribution diagrams of the optically controlled multi-gate thyristor at 0, 80, and 600 ns in the circuit.

    图 14  A模式验证测试结构

    Fig. 14.  Verification test structure for Mode A.

    图 15  A模式验证测试波形

    Fig. 15.  Verification test waveform for Mode A.

    图 16  C模式下测试电路

    Fig. 16.  Test circuit in Mode C.

    图 17  C模式下电压电流波形

    Fig. 17.  Voltage and current waveforms in Mode C.

    图 18  B模式下测试电路

    Fig. 18.  Test circuit in Mode B.

    图 19  B模式下测试波形

    Fig. 19.  Test waveform in Mode B.

    图 20  基于不同模式特征完成的3种封装 (a) A模式特征器件封装; (b) B模式特征器件封装; (c) C模式特征器件封装

    Fig. 20.  Three packages based on different mode characteristics: (a) Mode A characteristic device Package; (b) Mode B characteristic device package; (c) Mode C characteristic device package.

    图 21  基于开关的多模式特征研制的器件开展的典型应用验证 (a)多路同步固态起爆器应用; (b) KDP光开关驱动脉冲源应用

    Fig. 21.  Typical application verification of devices developed based on multi-mode switch characteristics: (a) Multi-channel synchronous solid-state initiator application; (b) KDP optical switch drive pulse source application.

    表 1  激光参数与开关典型参数实验数据表

    Table 1.  Experimental data table of laser parameters and typical switch parameters.

    激光功率
    /MW
    激光能量
    /mJ
    充电电压
    /kV
    电压下降
    时间/ns
    电流峰值
    /kA
    电流上升
    时间/ns
    导通延迟
    时间/ns
    电流脉冲
    宽度/ns
    开关峰值
    功率/MW
    功率比值/N di/dt/(kA
    ·μs-1)
    2.16 21.6 4.5 44.3 10.54 67.2 13.5 652 47.4 22 157
    1.92 19.2 4.5 44.6 10.54 67.3 12.6 654 47.4 25 157
    1.68 16.8 4.5 45.4 10.48 65.3 12.1 665 47.2 28 160
    1.47 14.7 4.5 45.4 10.42 66.4 11 667 46.9 32 157
    1.32 13.2 4.5 46.3 10.34 64.3 10.1 661 46.5 35 161
    1.08 10.8 4.5 48.6 10.35 68 8.88 663 46.6 43 152
    0.87 8.7 4.5 50.2 10.07 71.6 10.2 684 45.3 52 141
    0.678 6.78 4.5 46 9.71 65.1 13.7 742 43.7 64 149
    0.6 6 4.5 47.4 9.71 65.1 13.5 742 43.7 73 149
    0.54 5.4 4.5 52.5 9.41 62.7 13.5 765 42.3 78 150
    0.46 4.6 4.5 60.3 9.17 63.3 13.4 795.6 41.3 90 145
    0.39 3.9 4.5 68 8.62 63 14.1 832 38.8 99 137
    0.3 3 4.5 128 8.52 70.5 15.4 829 38.3 128 121
    0.24 2.4 4.5 158.4 8.48 95.8 18.6 835 38.2 159 89
    0.162 1.62 4.5 196 8.39 130.4 25.9 842 37.8 233 64
    0.072 0.72 4.5 221 8.13 222 52.6 857 36.6 508 37
    0.057 0.57 4.5 254 8.23 199 96 848 37.0 650 41
    0.0474 0.474 4.5 249.7 8.23 202 102 850 37.0 781 41
    0.0438 0.438 4.5 263 8.22 197.8 108 869 37.0 845 42
    0.0372 0.372 4.5 265 8.19 208.9 119 858 36.9 991 39
    0.0312 0.312 4.5 278 8.17 218 133 852 36.8 1178 37
    0.0252 0.252 4.5 252 8.16 212 153 874 36.7 1457 38
    0.0186 0.186 4.5 251 8.13 203 181 878 36.6 1967 40
    0.0126 0.126 4.5 271 7.97 212 276 897 35.9 2846 38
    0.0048 0.048 4.5 351 7.78 245 406 955 35.0 7294 32
    下载: 导出CSV

    表 2  器件驱动激光能量、短路电流、开通前沿的关系

    Table 2.  The relationship between device drive laser energy, short-circuit current, and turn-on edge.

    激光能量/mJ工作电压/kV短路电流/kA电流前沿
    /ns
    电流脉宽
    /ns
    di/dt
    /(kA·μs–1)
    0.941.8866.875.028
    2.143.424049.086
    2.643.7536.646.0102
    3.645.6520.436.7277
    4.645.8418.836.0311
    5.446.4818.938.0343
    6.34718.737.7374
    7.447.318.638.7392
    8.547.9118.638.3425
    下载: 导出CSV

    表 3  不同电压下开关的导通特性

    Table 3.  The conduction characteristics of the switch at different voltages.

    激光
    能量/μJ
    工作
    电压
    /kV
    短路
    电流/kA
    电流
    前沿
    /ns
    di/dt
    /
    (kA·μs–1)
    2005.02.012816
    2006.02.812123
    2007.03.911833
    2008.05.411149
    2008.56.011055
    下载: 导出CSV
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出版历程
  • 收稿日期:  2024-11-19
  • 修回日期:  2025-01-10
  • 上网日期:  2025-01-14

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