RF Breakdown Limits

Author(s):  
Robert A. Jameson
Keyword(s):  
2010 ◽  
Vol 130 (12) ◽  
pp. 1073-1080
Author(s):  
Norihiko Sasaki ◽  
Mitsuharu Nogaku ◽  
Yutaka Uchida

1975 ◽  
Vol 11 (2) ◽  
pp. 423-426 ◽  
Author(s):  
C. Varmazis ◽  
T. Luhman ◽  
A. Joshi ◽  
O. Kammerer ◽  
S. Giordano ◽  
...  

Author(s):  
I.N. Onishchenko ◽  
V.A. Balakirev ◽  
Y.P. Bliokh ◽  
G.V. Sotnikov
Keyword(s):  

2010 ◽  
Author(s):  
Y. Jiang ◽  
A. Vikharev ◽  
M. A. LaPointe ◽  
J. L. Hirshfield ◽  
Steven H. Gold ◽  
...  
Keyword(s):  

Author(s):  
X. Xu ◽  
R.S. Callin ◽  
W.R. Fowkes ◽  
A. Menegat ◽  
G.P. Scheitrum ◽  
...  
Keyword(s):  
X Band ◽  

1986 ◽  
Vol 68 ◽  
Author(s):  
Brian E. Thompson ◽  
Herbert H. Sawun ◽  
Aaron Owens

AbstractContinuity equations for the concentration of electrons, positive ions, and negative ions were constructed and solved to predict rf breakdown voltages and the electrical properties of SF, discharges.These balances for the three types of charged species include terms for convection (electric field-driven fluxes), diffusion, and reactions (ionization, electron attachment, and negative-positive ion recombination).The mobilities, diffusivities, and reaction rate coefficients necessary for the rf discharge model are based on reported measurements and calculations of these parameters in dc electric fields.The electric fields developed in the rf discharge are calculated from Poisson's equation and applied voltage conditions.Predictions based on this model are compared with measured rf breakdown characteristics of SF6.


2018 ◽  
Vol 46 (4) ◽  
pp. 900-908 ◽  
Author(s):  
Yibing Cao ◽  
Jun Sun ◽  
Yuchuan Zhang ◽  
Zhimin Song ◽  
Ping Wu ◽  
...  

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