1985
DOI: 10.1063/1.1138504
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1000-V, 300-ps pulse-generation circuit using silicon avalanche devices

Abstract: A Marx configured avalanche transistor string and a pulse rise-time peaking diode are used to generate pulses of >1000 V into a 50-Ω load with rise times of less than 300 ps. The trigger delay of this circuit is about 7–10 ns, with jitter <100 ps. This circuit has been used to generate pulses at a repetition rate up to 5 kHz.

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Cited by 47 publications
(27 citation statements)
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“…6,7,9,11,12 In both cases we deal with a collective phenomenon of superfast propagation. It is based on avalanche multiplication of the already existing carriers due to impact ionization in a finite narrow region of the device, followed by screening of the electrical field due to Maxwell relaxation in the adjacent spatial region.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…6,7,9,11,12 In both cases we deal with a collective phenomenon of superfast propagation. It is based on avalanche multiplication of the already existing carriers due to impact ionization in a finite narrow region of the device, followed by screening of the electrical field due to Maxwell relaxation in the adjacent spatial region.…”
Section: Discussionmentioning
confidence: 99%
“…1 In this article we demonstrate that the threshold of tunneling ionization in the bulk of a Si p ϩ -n -n ϩ structure can be reached under the same experimental conditions as for triggering impact ionization fronts. [6][7][8][9] Typically an ionization front is triggered by applying a voltage pulse with a steep slope (у1 kV/ns) to the p ϩ -n -n ϩ structure in reverse direction. 6,9,10 In structures with kilovolt pϪn junctions and large cross-sections, this process is used for sharpening electrical pulses.…”
Section: Introductionmentioning
confidence: 99%
“…Возможность сверхбыстрого -субнаносекундного переключения из блокирующего в проводящее состоя-ние высоковольтной кремниевой диодной p + N 0 n + -струк-туры была показана в [1,2], а затем подтверждена в [3]. После этого был проведен большой комплекс исследова-ний, в результате которых диодный лавинный переклю-чатель -обостритель высоковольтных импульсов стал широко используемым прибором мощной импульсной техники субнаносекундного диапазона.…”
unclassified
“…[1][2][3][4][5][6][7][8][9] The front passage fills the structure with dense electron-hole plasma and hence leads to the transition of the reversely biased p-n junction from lowconducting to high conducting state. Apart from microwave TRAPATT ͑TRApped Plasma Avalanche Triggered Transit͒ diodes 1,2 triggering of impact ionization fronts has been observed in high-voltage p + -n-n + diodes manufactured from both Si ͑Refs.…”
Section: Introductionmentioning
confidence: 99%
“…[3][4][5][6][7][8][9] In the respective limiting case v f / v s + 1 the effect of transport asymmetry vanishes. As it follows from Eqs.…”
mentioning
confidence: 99%