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

追逐

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

虚假

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.

Ethics

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.

Ordnance

Was ich nicht weiß, macht mich nicht heiß?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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