2010
DOI: 10.1017/s0022377810000644
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Theory of azimuthal surface waves propagating in non-uniform waveguides

Abstract: This paper is devoted to the theory of surface waves propagating across axis of symmetry in non-uniform cylindrical metal waveguides with plasma filling. The presented results are devoted to: first, studying an influence of plasma density non-uniformity on the features of these waves; second, studying an influence of an external magnetic fields' non-uniformity on their dispersion properties; third, studying possibility to sustain gas discharge by propagation of these waves under different operating regimes. Th… Show more

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Cited by 22 publications
(33 citation statements)
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“…In the case, when flows of charged particles are absent in the region R 2 > r > R 1 (it means j r = j ϕ = 0 and hence F b = 0) expressions for the AMs coincide with that are obtained in [6] for studying dispersion properties of these modes in the case of a dense plasma (Langmuir frequency is larger than electron cyclotron frequency). Thus for tangential components of the AMs fields one can derive the following expressions in the region occupied by the electron beam:…”
Section: Basic Equationssupporting
confidence: 60%
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“…In the case, when flows of charged particles are absent in the region R 2 > r > R 1 (it means j r = j ϕ = 0 and hence F b = 0) expressions for the AMs coincide with that are obtained in [6] for studying dispersion properties of these modes in the case of a dense plasma (Langmuir frequency is larger than electron cyclotron frequency). Thus for tangential components of the AMs fields one can derive the following expressions in the region occupied by the electron beam:…”
Section: Basic Equationssupporting
confidence: 60%
“…the AMs propagating in the considered waveguide (see [6]) under the condition of α b = 0 (that means absence of the beam), R j = r j Ω e c −1 is dimensionless radial co-ordinate of the j-th particle of the beam. It is suitable for formulate momentum equation, which describes the beams' electrons motion, using terms of their impulses p = γm e V (γ is relativistic factor), because it allows one to take into the account a weak relativism of the beam:…”
Section: Basic Equationsmentioning
confidence: 99%
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