2005
DOI: 10.1109/tps.2005.856533
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Temporal structure of the fast electron beam generated in the pseudospark discharge with external triggering

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Cited by 16 publications
(8 citation statements)
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“…The studies were conducted as a assemble design with a simple electrode system consisting of a hollow cathode and the anode with a hole on the axis [11,12] and at a sealed-off pseudospark switches series of prototypes TDI [2]. In some cases, cathodes divided were used, allowing current to record the current on different parts of the electrodes.…”
Section: Experimental Equipment and Methodicsmentioning
confidence: 99%
“…The studies were conducted as a assemble design with a simple electrode system consisting of a hollow cathode and the anode with a hole on the axis [11,12] and at a sealed-off pseudospark switches series of prototypes TDI [2]. In some cases, cathodes divided were used, allowing current to record the current on different parts of the electrodes.…”
Section: Experimental Equipment and Methodicsmentioning
confidence: 99%
“…Interpretation of the processes in the stage of the delay time to breakdown have been carried out in numerous papers [2,12,14,[64][65][66][67][68][69]. The physical model for the low-pressure discharge formation at the prebreakdown stage has been proposed and developed in [2,12,14].…”
Section: Discharge Development At the Stage Of Delay Time To Breakdownmentioning
confidence: 99%
“…The electron beams are obtained in the single gap or multi-gap electrode systems where the anode plates have central bore holes. A variety of experimental data on the investigation of the process of the beam generation and on the applications of the beams has been presented in the current literature [12,39,65,[71][72][73][74][75]. In most cases, the beam is produced at the stage of delay time to breakdown.…”
Section: Discharge Development At the Stage Of Delay Time To Breakdownmentioning
confidence: 99%
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“…The low-pressure discharge in a narrow gap exposed to such high voltage is characterized as a discharge existing under a strong overvoltage regime with the magnitude of the reduced electric field E/N > 10 5 Td. Such a huge electric field in the gap provides the appearance of so-called runaway electrons [10][11][12][13][14] effectively forming the emergent e-beam with the energy close to the applied voltage. The breakdown process of the strongly overvoltage open discharge (SOOD) cannot be described by the concept of Townsend electron avalanches.…”
Section: Introductionmentioning
confidence: 99%