2019
DOI: 10.1088/1361-6595/ab2230
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Filamentary nanosecond surface dielectric barrier discharge. Plasma properties in the filaments

Abstract: Streamer-to-filament transition is a general feature of nanosecond discharges at elevated pressure. The transition is observed in different discharges by different groups: in the nanosecond surface dielectric barrier discharges (nSDBDs) in a single shot regime at high pressure (2-15 bar), in the point-to-point or point-to-plane open electrodes discharges at high repetitive frequency (so-called nanosecond repetitive pulsed discharges, NRPDs) at atmospherics pressure. The present paper contains experimental anal… Show more

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Cited by 57 publications
(117 citation statements)
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References 37 publications
(95 reference statements)
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“…It was suggested [26] that such a slow decay of the electron density is due to fact that plasma in the filaments is close to local thermal equilibrium (LTE); the gas temperature in the discharge is a few electronvolts, and the dynamics of plasma decay is determined mainly by gas cooling. This idea is developing in [27], where a kinetic model is suggested to provide a sharp, parts of nanoseconds, transition from streamer to filamentary plasma. Analysis of surface charge per streamer and per filament shows that for both polarities, the charge per filament accumulated on the surface is at least one order of magnitude higher than the charge per streamer [28].…”
Section: Electron Density and Surface Chargementioning
confidence: 99%
“…It was suggested [26] that such a slow decay of the electron density is due to fact that plasma in the filaments is close to local thermal equilibrium (LTE); the gas temperature in the discharge is a few electronvolts, and the dynamics of plasma decay is determined mainly by gas cooling. This idea is developing in [27], where a kinetic model is suggested to provide a sharp, parts of nanoseconds, transition from streamer to filamentary plasma. Analysis of surface charge per streamer and per filament shows that for both polarities, the charge per filament accumulated on the surface is at least one order of magnitude higher than the charge per streamer [28].…”
Section: Electron Density and Surface Chargementioning
confidence: 99%
“…Stark broadening was also used for electron number density measurement in several works in pin-to-pin or pinto-plane configuration [16][17][18][19] and all authors reported electron number densities higher than 10 18 cm -3 . Such a high electron number density was also reported in SDBD discharges [20][21][22]. The authors demonstrated that the increase of pressure can be responsible for the transition from a weakly ionized plasma (called "streamer") to a fully-ionized plasma (called "filament").…”
Section: Introductionmentioning
confidence: 53%
“…This was already seen when the excited states of molecular nitrogen were included in Ref. [21]. New simulations are performed changing the number of nitrogen and oxygen excited states included in the chemical mechanism.…”
Section: Influence Of the Number Of Atomic States In The Modelmentioning
confidence: 82%
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