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On the theory of stationary waves in plasmas

✍ Scribed by N.G. Van Kampen


Publisher
Elsevier Science
Year
1955
Weight
720 KB
Volume
21
Category
Article
ISSN
0031-8914

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✦ Synopsis


Existing theories of stationary plasma oscillations lead to a dispersion equation ( ), involving an integration across a pole. It is here shown that this difficulty is of purely mathematical origin, and can be overcome by a proper treatment. This treatment leads to a complete set of stationary solutions, which are much more numerous than the usual plasma oscillations. In particular, their wave lengths and frequencies are not connected by a dispersion equation, but independently assume all real values. Special superpositions of these stationary solutions correspond to the usual plasma oscillations. They constitute slightly damped plane waves, which do obey the dispersion equation ( ), the integral being interpreted as a Cauchy principal value. An arbitrary initial distribution behaves (after a short transient time) like a superposition of such waves, as far as the density is concerned.


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Quasi-stationary solitons for Langmuir w
✍ Anjan Biswas πŸ“‚ Article πŸ“… 2009 πŸ› Elsevier Science 🌐 English βš– 142 KB

The multiple-scale perturbation analysis is used to study the perturbed nonlinear Schro Β¨dinger's equation, that describes the Langmuir waves in plasmas. The perturbation terms include the non-local term due to nonlinear Landau damping. The WKB type ansatz is used to define the phase of the soliton