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Example text

W e cannot be certain, therefore, that the differences in spectra observed by the other authors were directly related to the frequency of the exciting s y s t e m . The differences in the behavior of electrical parameters of high-frequency and DC discharges b e c o m e apparent only at high frequencies and relatively low gas p r e s s u r e s . It would thus frequency appear that in c a s e s where ω

In a narrow tube the positive ions and electrons reach the walls in l e s s time than they do in a wide tube. The result is a higher recombination rate, which must be compensated for by increasing the number of excitation events which in turn involves a higher longitudinal field gradient. In a narrow tube a major influence is the transverse field g e n erated by negative charges on the w a l l s , which are stored up as the wall is bombarded by electrons drifting toward it. The c r o s s field effect produces a curvature in the equipotential surfaces; the latter b e c o m e convex, protruding toward the cathode.

Discharge When working with frequencies above 2500 M c / s , the tube is installed in a waveguide. determines the distinctive characteristics The type of coupling of a high-frequency discharge, since it determines the amount of power that can be fed to the discharge gap. Conventionally, two types of high-frequency discharge are distinguished at low p r e s s u r e s : glow discharge and ring discharge [22, 1 7 2 ] . High-frequency glow discharge This is generated in a gap connected to a high-frequency circuit through internal will see or external e l e c t r o d e s .

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