Similarity law for rf breakdown
dc.contributor.author | Lisovskiy, V. | |
dc.contributor.author | Booth, Jean-Paul | |
dc.contributor.author | Landry, K. | |
dc.contributor.author | Douai, D. | |
dc.contributor.author | Cassagne, V. | |
dc.contributor.author | Yegorenkov, V. | |
dc.date.accessioned | 2010-11-17T18:03:46Z | |
dc.date.available | 2010-11-17T18:03:46Z | |
dc.date.issued | 2008-04 | |
dc.description.abstract | This paper demonstrates that the similarity law for the rf gas breakdown has the form Urf =F(p ·L, L/R, f ·L)(where Urf is the rf breakdown voltage, p is the gas pressure, L and R are the length and diameter of the discharge tube, respectively, f is the frequency of the rf electric field). It means that two rf breakdown curves registered for narrow inter-electrode gaps or in geometrically similar tubes and depicted in the Urf (p ·L) graph will coincide only when the condition f ·L = const is met. This similarity law follows from the rf gas breakdown equation and it is well supported by the results of measurements. | en |
dc.description.sponsorship | - | en |
dc.identifier.citation | Europhysics Letters, 82 (2008) 15001 | en |
dc.identifier.uri | https://ekhnuir.karazin.ua/handle/123456789/1696 | |
dc.language.iso | en | en |
dc.publisher | www.epl journal.org | en |
dc.relation.ispartofseries | ;doi: 10.1209/0295-5075/82/15001 | |
dc.subject | plasma physics | en |
dc.subject | gas discharges | en |
dc.title | Similarity law for rf breakdown | en |
dc.type | Article | en |
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