Abstract

In this paper, the positive and negative symmetric pulses with a fast rising edge were generated by a GaAs photoconductive semiconductor switch (PCSS). When the GaAs PCSS was biased at 2.0 kV and triggered by a femtosecond laser pulse with a pulse energy of 97.5 J, the peak voltages of the positive and negative pulses were 1.313 kV and 1.329 kV, respectively, and the rise times were 174 ps and 164 ps, respectively. Moreover, the GaAs PCSS presents good stability. The experimental results show that GaAs PCSSs can meet the requirement of a femtosecond streak camera.

Highlights

  • GaAs photoconductive semiconductor switches (PCSSs) have many advantages, including fast response times, high repetition rates, simple mechanical structure and low jitter [1,2,3,4]

  • When femtosecond laser pulses are focused on the gap of GaAs PCSSs, photo-excited carries are generated at the semiconductor’s conduction band, and are subsequently accelerated by a bias electrical field, and terahertz waves are radiated at the same time [8,9,10]

  • A sweep circuit was designed, in which a GaAs PCSS was used as an ultrafast pulse generator, positive and negative symmetric pulses output was realized, and the performance was tested

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Summary

Introduction

GaAs photoconductive semiconductor switches (PCSSs) have many advantages, including fast response times, high repetition rates (in the order of GHz), simple mechanical structure and low jitter [1,2,3,4]. When femtosecond laser pulses are focused on the gap of GaAs PCSSs, photo-excited carries are generated at the semiconductor’s conduction band, and are subsequently accelerated by a bias electrical field, and terahertz waves are radiated at the same time [8,9,10]. The slope of sweep voltage decides the sweep speed of stripe tube, dictating the stripe tube’s temporal resolution. The stripe tube’s temporal resolution in integral mode rests with the jitter time of the sweep circuit. A sweep circuit was designed, in which a GaAs PCSS was used as an ultrafast pulse generator, positive and negative symmetric pulses output was realized, and the performance was tested. The device can be applied in femtosecond streak cameras, and the scanning speed and temporal resolution can be expected to be improved

Experimental Setup
The bottom is part of the and the shown in Figure
Results and Discussion
Conclusions

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