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Revision of “Cumulative effect of the filamentation and Weibel instabilities in counterstreaming thermal plasmas” [Phys. Plasmas13, 102107 (2006)]
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10.1063/1.2830646
/content/aip/journal/pop/15/1/10.1063/1.2830646
http://aip.metastore.ingenta.com/content/aip/journal/pop/15/1/10.1063/1.2830646
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Two shells of counterstreaming plasma, and the filamentation mode with wave vector perpendicular to the streaming direction.

Image of FIG. 2.
FIG. 2.

Filamentation instability in a counterstreaming plasma for three values of electron streaming speed: (solid line), (dashed line), and (dotted line). The coordinates are and .

Image of FIG. 3.
FIG. 3.

Weibel instability in a bi-Maxwellian plasma for three values of the electron anisotropy : (solid line), (dashed line), and (dotted line). The coordinates are and .

Image of FIG. 4.
FIG. 4.

The cumulative effect (growth rates with solid line) for the Weibel and filamentation instabilities in a counterstreaming electron plasma, with , and a bi-Maxwellian distribution, with , and . The growing rates of the Weibel instability (dotted line) and filamentation instability (dashed line) are shown using the same parameters. ( and .)

Image of FIG. 5.
FIG. 5.

The same as in Fig. 4, but with , , and .

Image of FIG. 6.
FIG. 6.

The same as in Fig. 4, but with , , and . Weibel instability does not exist along the propagation direction of filamentation instability, but the unstable mode is supressed (solid line) by the cumulative effect.

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2008-01-10
2014-04-24
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Revision of “Cumulative effect of the filamentation and Weibel instabilities in counterstreaming thermal plasmas” [Phys. Plasmas13, 102107 (2006)]
http://aip.metastore.ingenta.com/content/aip/journal/pop/15/1/10.1063/1.2830646
10.1063/1.2830646
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