2010
DOI: 10.3103/s106287381002019x
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Influence of thin dielectric layers on electron emission and plasma-surface contact stability

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Cited by 12 publications
(5 citation statements)
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“…Thermionic emission from hot metals [15] and photoemission from sunlight exposure [16] can induce a "strong" emitted flux Γ emit that exceeds the influx of electrons from the plasma Γ ep . Secondary emission coefficients γ ≡ Γ emit /Γ ep can exceed unity for metal surfaces [17] at high plasma temperatures while dielectric surfaces or oxide film coated electrodes [18] have significantly higher emission yields which can enable γ > 1 at more modest temperatures. For any emission type when γ > 1, the zero current condition cannot be met unless some of the emission is returned to the wall by a barrier field (Γ eret > 0).…”
mentioning
confidence: 99%
“…Thermionic emission from hot metals [15] and photoemission from sunlight exposure [16] can induce a "strong" emitted flux Γ emit that exceeds the influx of electrons from the plasma Γ ep . Secondary emission coefficients γ ≡ Γ emit /Γ ep can exceed unity for metal surfaces [17] at high plasma temperatures while dielectric surfaces or oxide film coated electrodes [18] have significantly higher emission yields which can enable γ > 1 at more modest temperatures. For any emission type when γ > 1, the zero current condition cannot be met unless some of the emission is returned to the wall by a barrier field (Γ eret > 0).…”
mentioning
confidence: 99%
“…For example, sheath potential for tokamaks varies from few to hundreds volts, but electric field strength depending on plasma density and electron temperature can be as high as 10 7 V/m [1]. Additional electron emission into plasma can change sheath potential, thus influencing plasma faced materials (PFM) by sputtering, and in some cases leads to the plasma-surface instabilities [2]. The increase of the surface emissivity correlates also with the probability of unipolar arcs ignition [3] resulting in plasma pollution with impurities.…”
Section: Introductionmentioning
confidence: 99%
“…As far as there are no strong evidences that the reason of such currents is classical field emission due to field enhancement on sharp surface relief, it was named as low-field emission (LFE) [2]. Electron emission into plasma can change sheath potential, thus influencing plasma facing materials by sputtering, and in some cases leads to the plasma-surface instabilities [3]. The total current of LFE from the wall in general is much lower, compared with that of secondary ion-electron emission, but local current density can be rather high as electrons emit from small emission sites.…”
Section: Introductionmentioning
confidence: 99%