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A solid-state pulsed power generator has been developed. It is based on Blumlein pulse forming network (PFN) combined with saturable pulse transformer (SPT). The primary circuit is switched by a switching unit consisting of three MOS-gated thyristors connected in parallel. The SPT functions both as a transformer to increase the voltage and as a closing switch for the secondary circuit. The PFN on the secondary side is charged by the transformer and switched by the SPT so that a pulsed output is generated on a matched load. In the demonstration experiment using one module, an output with peak voltage of ~10.4 kV and pulsewidth of ~160 ns was obtained on a resistive load of $52~\Omega $. Furthermore, three identical modules, sharing a common primary circuit, have been connected in series to demonstrate voltage adding, where a peak output voltage of ~30 kV was obtained on a load of $156~\Omega $ with energy efficiency of ~54 %. This pulsed power generator has been tested at repetition rate of 20 kHz in burst mode. [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]