• High Power Laser and Particle Beams
  • Vol. 36, Issue 4, 043022 (2024)
Mingxuan Gao1, Yang Zhang1、*, and Jun Zhang2
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China
  • 2College of Science, National University of Defense Technology, Changsha 410073, China
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    DOI: 10.11884/HPLPB202436.230236 Cite this Article
    Mingxuan Gao, Yang Zhang, Jun Zhang. Influence of high-power microwave signal on temperature distribution of PIN limiter[J]. High Power Laser and Particle Beams, 2024, 36(4): 043022 Copy Citation Text show less
    Field-circuit collaborative simulation model of two-stage PIN limiter
    Fig. 1. Field-circuit collaborative simulation model of two-stage PIN limiter
    Structure and doping concentration of the first stage PIN diode
    Fig. 2. Structure and doping concentration of the first stage PIN diode
    Structure and doping concentration of the second stage PIN diode
    Fig. 3. Structure and doping concentration of the second stage PIN diode
    Curve of the two PIN diodes’ temperature distribution inside the limiter at the moment its maximum temperature reaches the melting point of silicon
    Fig. 4. Curve of the two PIN diodes’ temperature distribution inside the limiter at the moment its maximum temperature reaches the melting point of silicon
    Temperature distribution under different amplitude (local)
    Fig. 5. Temperature distribution under different amplitude (local)
    Temperature distribution under different frequency (local)
    Fig. 6. Temperature distribution under different frequency (local)
    Normalized dissipation power distribution under the action of signals with different amplitude at the moment the limiter’s maximum temperature reaches the melting point of silicon (local)
    Fig. 7. Normalized dissipation power distribution under the action of signals with different amplitude at the moment the limiter’s maximum temperature reaches the melting point of silicon (local)
    Electron and hole concentration distribution at different moments in a signal cycle
    Fig. 8. Electron and hole concentration distribution at different moments in a signal cycle
    Electric field distribution at different moment in the signal cycle
    Fig. 9. Electric field distribution at different moment in the signal cycle
    Current density distribution at different moment in the signal cycle
    Fig. 10. Current density distribution at different moment in the signal cycle
    Normalized electric field distribution under the action of signals with different amplitude at the moment the limiter’s maximum temperature reaches the melting point of silicon (local)
    Fig. 11. Normalized electric field distribution under the action of signals with different amplitude at the moment the limiter’s maximum temperature reaches the melting point of silicon (local)
    voltage/Vwidth of high-temperature area/μm
    4006.6
    5006.9
    6007.3
    7007.6
    8007.9
    9008.1
    10008.3
    Table 1. Width of high-temperature area under different amplitude
    Mingxuan Gao, Yang Zhang, Jun Zhang. Influence of high-power microwave signal on temperature distribution of PIN limiter[J]. High Power Laser and Particle Beams, 2024, 36(4): 043022
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