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Nonlinear interactions of positive and negative energy modes in rarefied plasmas (I)
The nonlinear interactions of electrostatic modes in a plasma are studied within the framework of the weak-turbulence approximation. It is shown that the multi-wave interaction (resonant mode-mode coupling) can be explosively unstable when, for Σ j=1 n k j = 0 and Σ j=1 n ω k j = 0, we also have S 1...
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Published in: | Annals of physics 1969-11, Vol.55 (2), p.207-247 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The nonlinear interactions of electrostatic modes in a plasma are studied within the framework of the weak-turbulence approximation. It is shown that the multi-wave interaction (resonant mode-mode coupling) can be explosively unstable when, for
Σ
j=1
n
k
j
= 0 and
Σ
j=1
n
ω
k
j
= 0, we also have
S
1 =
S
2 = … =
S
n
, where
S
j = (
∂ϵ
∂ω
kj
)
/|
∂ϵ
∂ω
kj
|
,
n being the number of interacting waves and ϵ the dielectric constant.
Significant examples are analyzed with special consideration for that of a plasma with a loss-cone distribution in a strong magnetic field
B. This in fact can have positive and negative energy modes, for which unstable three-wave interactions can occur with growth rates which are appreciable for rather modest intensities. The modes considered are of flute type, with
k · B = 0, so that convection along the lines of force does not affect the validity of the above results. A nonlinear mechanism of the type analyzed here can provide a possible explanation of the bursts of radiation often associated with low-density mirror confined plasmas. |
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ISSN: | 0003-4916 1096-035X |
DOI: | 10.1016/0003-4916(69)90178-X |