In this paper we present our solid-state nanosecond pulse source (the solid-state impedance-matched Marx generator) which can generate arbitrary waveforms and which can be used for pulsed discharge generation. The purpose of the development of such a generator is twofold: by being able to change the waveform at will, we aim to control the discharge generated by such pulses very precisely which can be very useful for plasma applications, but also for more fundamental studies. In the presented study, we applied the arbitrary-waveform pulse source for streamer discharge generation in a cylinder-wire-like arrangement and used the arbitrary-waveform capability to change the rise time (in our experiments we used 6.8-26.2 ns) of unipolar positive ...
In this paper, we present the final implementation of our 0-50-kV picosecond rise time 0.5-10-ns pul...
We use (sub)nanosecond high-voltage pulses to generate streamers in atmospheric-pressure air in a wi...
In this paper, we present the final implementation of our 0-50-kV picosecond rise time 0.5-10-ns pul...
In this paper we present our solid-state nanosecond pulse source (the solid-state impedance-matched ...
In this paper we present our solid-state nanosecond pulse source (the solid-state impedance-matched ...
In this paper we present our solid-state nanosecond pulse source (the solid-state impedance-matched ...
In this paper we present our solid-state nanosecond pulse source (the solid-state impedance-matched ...
In this paper we present our solid-state nanosecond pulse source (the solid-state impedance-matched ...
Streamer discharges generated by nanosecond high-voltage pulses have gained attraction for a variety...
Streamer discharges generated by nanosecond high-voltage pulses have gained attraction for a variety...
Streamer discharges generated by nanosecond high-voltage pulses have gained attraction for a variety...
Streamer discharges generated by nanosecond high-voltage pulses have gained attraction for a variety...
Streamer discharges generated by nanosecond high-voltage pulses have gained attraction for a variety...
In this paper, we present the final implementation of our 0-50-kV picosecond rise time 0.5-10-ns pul...
In this paper, we present the final implementation of our 0-50-kV picosecond rise time 0.5-10-ns pul...
In this paper, we present the final implementation of our 0-50-kV picosecond rise time 0.5-10-ns pul...
We use (sub)nanosecond high-voltage pulses to generate streamers in atmospheric-pressure air in a wi...
In this paper, we present the final implementation of our 0-50-kV picosecond rise time 0.5-10-ns pul...
In this paper we present our solid-state nanosecond pulse source (the solid-state impedance-matched ...
In this paper we present our solid-state nanosecond pulse source (the solid-state impedance-matched ...
In this paper we present our solid-state nanosecond pulse source (the solid-state impedance-matched ...
In this paper we present our solid-state nanosecond pulse source (the solid-state impedance-matched ...
In this paper we present our solid-state nanosecond pulse source (the solid-state impedance-matched ...
Streamer discharges generated by nanosecond high-voltage pulses have gained attraction for a variety...
Streamer discharges generated by nanosecond high-voltage pulses have gained attraction for a variety...
Streamer discharges generated by nanosecond high-voltage pulses have gained attraction for a variety...
Streamer discharges generated by nanosecond high-voltage pulses have gained attraction for a variety...
Streamer discharges generated by nanosecond high-voltage pulses have gained attraction for a variety...
In this paper, we present the final implementation of our 0-50-kV picosecond rise time 0.5-10-ns pul...
In this paper, we present the final implementation of our 0-50-kV picosecond rise time 0.5-10-ns pul...
In this paper, we present the final implementation of our 0-50-kV picosecond rise time 0.5-10-ns pul...
We use (sub)nanosecond high-voltage pulses to generate streamers in atmospheric-pressure air in a wi...
In this paper, we present the final implementation of our 0-50-kV picosecond rise time 0.5-10-ns pul...