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Particle-in-cell simulations of the runaway breakdown of nitrogen
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10.1063/1.4769748
/content/aip/journal/jap/112/11/10.1063/1.4769748
http://aip.metastore.ingenta.com/content/aip/journal/jap/112/11/10.1063/1.4769748
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

(a) Temporal evolution of the RAE beam injected into the CA gap and reaching the anode at different cathode potentials; (b) electron energy distribution function at the anode at different cathode potentials; (c) and (d) potential distributions in the CA gap at different times at = 1.5 kV and = 10 kV, respectively. RC = 3 μm, τ = 70 ps, and Nmax = 106.

Image of FIG. 2.
FIG. 2.

(a) Comparison between RAE beam injected into the CA gap and RAE beam reaching the anode at Nmax  = 106 and Nmax  = 107 electrons; (b) electron energy distribution function at the anode at different amplitudes at Nmax  = 106 and Nmax  = 107 electrons; (c) potential distribution in the CA gap at different times at Nmax  = 107. RC  = 3 μm, τ = 100 ps, and = 1.5 kV.

Image of FIG. 3.
FIG. 3.

(a) Comparison between RAE beam injected into the CA gap and RAE beam reaching the anode at a different radius of the cathode; (b) electron energy distribution function at the anode at a different radius of the cathode; (c) and (d) potential distribution in the CA gap at different times for the case RC  = 3 μm. Nmax  = 107, τ = 100 ps, and  = 10 kV.

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/content/aip/journal/jap/112/11/10.1063/1.4769748
2012-12-14
2014-04-17
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Particle-in-cell simulations of the runaway breakdown of nitrogen
http://aip.metastore.ingenta.com/content/aip/journal/jap/112/11/10.1063/1.4769748
10.1063/1.4769748
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