1971
DOI: 10.1080/00207217108900330
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Plasma and electrode interactions in short gap discharges in air II. Electrode effects†

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Cited by 30 publications
(13 citation statements)
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“…Thus, the estimated lifetime in the range 30-60 nsec may be considered as the sum lifetime of consecutive randomly scattered 3 nsec (returning) emitting events. This interpretation is confirmed by the fact that for clean surfaces in air (and comparable surface conditions in vacuum) the authors who have worked with short-time cable discharges (to 5 1 nsec-20 nsec) report on emitting site lifetimes in the range of 1-5nsec (JOTTNEB [19,25,27,68, 761, GRAY, AUGIS (20,39,701). Thus, this representation again enforces the idea that the electron-phonon interaction model proposed here is applicable to such experimental conditions where type A microspot ensembles especially leave typical trumpet-like microcraters on the surface as described above (see Fig.…”
Section: Discussionsupporting
confidence: 65%
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“…Thus, the estimated lifetime in the range 30-60 nsec may be considered as the sum lifetime of consecutive randomly scattered 3 nsec (returning) emitting events. This interpretation is confirmed by the fact that for clean surfaces in air (and comparable surface conditions in vacuum) the authors who have worked with short-time cable discharges (to 5 1 nsec-20 nsec) report on emitting site lifetimes in the range of 1-5nsec (JOTTNEB [19,25,27,68, 761, GRAY, AUGIS (20,39,701). Thus, this representation again enforces the idea that the electron-phonon interaction model proposed here is applicable to such experimental conditions where type A microspot ensembles especially leave typical trumpet-like microcraters on the surface as described above (see Fig.…”
Section: Discussionsupporting
confidence: 65%
“…In the latter case it must be assumed that the 30 nm emitting sites are present in e great number on the surface. Obviously, this fact is the cause that the radial expansion of the cathode root or the damaged area is governed by the law of electronic diffusion (diffusion rate = 2/ploa0) of the current paths confirmed by the experiments of SLADE [14] and GUY [20] for such conditions. The cathode damage .due to this fast moving spot type is characterized by the appearence of the typical .trumpet-Iike microcraters with pronounced crater rims with diameters in the order ,of 0.5-2 pm described in the previous section.…”
Section: Discussionmentioning
confidence: 92%
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