2014
DOI: 10.1017/s0263034614000299
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Generation and radiation of ultra-wideband electromagnetic pulses with high stability and effective potential

Abstract: An ultra-wideband radiation source based on the excitation of a 64-element array of combined antennas by a generator of bipolar voltage pulses with the length of 1 ns, amplitude of 200 kV and pulse repetition rate of 100 Hz has been designed and studied. The peak power of the voltage pulse was 3.2 GW. The effective potential of the ultra-wideband source radiation reached 4.3 MV.

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Cited by 32 publications
(5 citation statements)
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“…This type of circuit is used both to charge coaxial lines and to form voltage pulses with subnanosecond rise times. The voltage rise time can be decreased from nanoseconds to tens of picoseconds with the use of peaking switches [9,28,29] and special diodes [30].…”
Section: Experimental Setupsmentioning
confidence: 99%
“…This type of circuit is used both to charge coaxial lines and to form voltage pulses with subnanosecond rise times. The voltage rise time can be decreased from nanoseconds to tens of picoseconds with the use of peaking switches [9,28,29] and special diodes [30].…”
Section: Experimental Setupsmentioning
confidence: 99%
“…But in the subnanosecond range, you can also get completely unique effects. For example, using shorter pulses to generate electromagnetic radiation allows to perform ultra-wideband radiolocation [15]. Subnanosecond electron beams and x-ray radiation are unique tools for studying the physics of the interaction of radiation with matter, when the pulse action time becomes comparable and even less than the characteristic times of some transition processes in gases and solids [16][17][18][19].…”
Section: Introductionmentioning
confidence: 99%
“…From the practical standpoint, these investigations are motivated by the need of creating ultrafast switches [28,29] and pulsed sources of electron, plasma, or x-ray beams [30][31][32]. It is also important to increase the breakdown strength of high-voltage gas feeder paths and shock-excited antenna systems [33]. In all of these studies, a special place is given to the phenomenon of electron runaway appearing at the breakdown delay stage [5,34].…”
Section: Introductionmentioning
confidence: 99%