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A pulsed-power generator based on the circuit scheme of a linear transformer driver (LTD) while using solid-state switches is referred to as a solid-state LTD (SSLTD). One of the advantages of the SSLTD compared with traditional pulsed-power generators is its flexibility in the output waveform. It has potential applications to atmospheric pressure gas discharge because this kind of discharge load usually exhibits a fast-changing impedance. In this paper, a feedback control system for SSLTDs is reported. It uses a system-on-chip analog-to-digital converter combined with a field programmable gate array. By using this system, our SSLTD has the ability to automatically adjust its output waveform based on the information obtained from the previous pulse. As a result, during repetitive operation, our SSLTD can figure out the right output waveform according to a user scenario and can respond to any variation that may occur on the load. [ABSTRACT FROM AUTHOR]

The low-voltage droop of high-voltage pulses is required to provide stable pulsed electric fields in many applications. Increasing the capacitance of energy storage capacitors increases both the size and the cost of the system. In this paper, four compensation stages based on the resonant circuit have been inserted into a 16-stage solid-state Marx generator to compensate for the voltage droop in different conditions. The nearly linear part of the sinusoidal voltage is precisely added to the load during discharging as compensation, and the rectangular pulsed voltage with little droop can be realized. Different numbers of compensation stages and different resonant inductances can compensate the droop to different levels, which means the compensation effect is also adjustable. Moreover, these compensation stages can operate as common stages in Marx generators as long as we open-circuit the resonant circuits. Since the capacitors in resonant compensation stages are also charged in parallel with capacitors in common stages, no auxiliary power supply is required. Simulating and experimental results show that the droop of a 9 kV pulse can be ideally compensated over a 500 Ω resistive load at various pulse widths. The pulse width should be shorter than the length of the nearly linear part of the sinusoidal voltage. [ABSTRACT FROM AUTHOR]