Volume 45 Issue 4
May  2016
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Xu Ming, Li Mengxia, An Xin, Bian Kangkang, Shi Wei. Infrared quenching operation of non-linear GaAs photoconductive semiconductor switch for terahertz generation[J]. Infrared and Laser Engineering, 2016, 45(4): 425001-0425001(5). doi: 10.3788/IRLA201645.0425001
Citation: Xu Ming, Li Mengxia, An Xin, Bian Kangkang, Shi Wei. Infrared quenching operation of non-linear GaAs photoconductive semiconductor switch for terahertz generation[J]. Infrared and Laser Engineering, 2016, 45(4): 425001-0425001(5). doi: 10.3788/IRLA201645.0425001

Infrared quenching operation of non-linear GaAs photoconductive semiconductor switch for terahertz generation

doi: 10.3788/IRLA201645.0425001
  • Received Date: 2015-08-23
  • Rev Recd Date: 2015-09-26
  • Publish Date: 2016-04-25
  • To use the non-linear GaAs photoconductive semiconductor switch (PCSS) with avalanche effect for terahertz generation, it is important to quench the photo-activated carrier domain (PACD) transporting in the semiconductor. In this work, a basic setup for quenching the non-linear GaAs PCSS was proposed which consists of two laser beams. The second laser beam was delayed about 100 ps for quenching the PACD after the first beam. In the experiments, the PCSS with 12 mm electrode gap can be biased up to 32 kV with 0.9 kA switching current. Good reproducibility of waveforms about 230 times at 20 kV is achieved with 14mm PCSS when trigger laser is orders of magnitude of tens milli-joules. Results show the process of infrared quenching non-linear mode could be operating repeatedly, which paves the way for future research of high power terahertz generation at high repetition rate.
  • [1] Xu Ming, Shi Wei, Hou Lei, et al. High current operation of a semi-insulating Gallium Arsenide photoconductive semiconductor switch triggering a spark gap[J]. Chin Phys Lett, 2010, 27(2):024212.
    [2] Shi Wei, Dai Huiying, Sun Xiaowei. Photo-activated charge domain in high-gain photoconductive switches[J]. Chinese Optics Letters, 2003, 1(9):553-555.
    [3] Shi Wei, Tian Liqiang. Mechanism analysis of periodicity and weakening surge of GaAs photoconductive semiconductor switches[J]. Appl Phys Lett, 2006, 89:202103.
    [4] Xu Ming, Shi Wei, Hou Lei, et al. Operation of pulse charged spark gap triggered by GaAs photoconductive semiconductor switch[J]. IEEE Trans Plasma Science, 2010, 38(10):2888-2893.
    [5] Mazzola M S, Schoenbach K H, Lakdawala V K, et al. Infrared queching of conductivity at high electric fields in a bulk, copper-compensated, optically activated GaAs switch[J]. IEEE Trans Electron Devices, 1990, 37(12):2499-2506.
    [6] Mar A, Serkland D K, Keeler D A, et al. Multi-filament triggering of PCSS for high current utilizing VCSEL triggers[C]//16th IEEE International Conference Pulsed Power, 2007:1000-1003.
    [7] Shi Wei, Qu Guanghui, Xu Ming, et al. Current limiting effects of photoactivated charge domain in semi-insulating GaAs photoconductive switch[J]. Appl Phys Lett, 2009, 94:072110.
    [8] Gunn J B. Properties of a free, steadily traveling electrical domain in GaAs[J]. IBM Journal of Research and Development, 1966, 10(4):300-309.
    [9] Gunn J B. Effect of domain and circuit properties on oscillations in GaAs[J]. IBM Journal of Research and Development, 1966, 10(4):310-320.
    [10] Shi Wei, Wang Xinmei, Hou Lei, et al. Design and performance of a high-gain double-layer GaAs photoconductive switch[J]. Acta Physica Sinica, 2008, 57(11):7185-7189.
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Infrared quenching operation of non-linear GaAs photoconductive semiconductor switch for terahertz generation

doi: 10.3788/IRLA201645.0425001
  • 1. Applied Physics Department,Xi'an University of Technology,Xi'an 710048,China

Abstract: To use the non-linear GaAs photoconductive semiconductor switch (PCSS) with avalanche effect for terahertz generation, it is important to quench the photo-activated carrier domain (PACD) transporting in the semiconductor. In this work, a basic setup for quenching the non-linear GaAs PCSS was proposed which consists of two laser beams. The second laser beam was delayed about 100 ps for quenching the PACD after the first beam. In the experiments, the PCSS with 12 mm electrode gap can be biased up to 32 kV with 0.9 kA switching current. Good reproducibility of waveforms about 230 times at 20 kV is achieved with 14mm PCSS when trigger laser is orders of magnitude of tens milli-joules. Results show the process of infrared quenching non-linear mode could be operating repeatedly, which paves the way for future research of high power terahertz generation at high repetition rate.

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