Titlebook: Gaseous Dielectrics VIII; Loucas G. Christophorou,James K. Olthoff Book 1998 Springer Science+Business Media New York 1998 Recycling.desig

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Low-Energy Electron Collision by Excited Atomsy in most low-temperature plasmas. Mechanisms underlying many phenomena in weakly ionized gas are based, in part, on the low-energy electron collisions with atoms and molecules. Ionization balance in partially ionized gas is maintained by a combination of excitation and ionization processes involvin

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From Corona Stabilization to Spark Breakdown in Point-To-Plane SF6 Gapsion and development. in SF., threshold voltages for spark breakdown under such conditions correspond to mean applied electric fields around 90 kV/cm/bar and people using such impulses to get high currents in gaseous gaps but without the risk of spark breakdown work with pulses generally of higher am

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Ionization and Ion Kinetics in c-C4F8ent ions, only CF.+ and C.F.+ react with neutral c-C.F., yielding C.F.+ as the major product ion with the rate coefficients of 4.7+0.5 and 3.3+0.5x10.cm.s., respectively. C.F.-and F-are formed by low energy electron attachment to C-C.F., and are inert to their parent gas molecule.

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The Dependence of Electron Capture Rate Constants on Electronic Polarizability different laboratories is observed. This could be caused either by not achieving the truly thermal distribution of electrons energy and/or not including the contribution from higher order electron attachment processes.

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Was ich nicht wei?, macht mich nicht hei??ere made at room temperature and cover the . range from 0.05 x 10. V cm. to 60 x 10.V cm. (0.05 Td to 60 Td, 1 Td = 10. V cm.). the electron attachment rate constant is virtually independent of . below about 50 x 10. V cm. and equal to ～ 13 x 10-. cm. s.. This small attachment rate constant may be due to impurities.

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