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Collisionless magnetohydrodynamics with gyrokinetic effects
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10.1063/1.2751601
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Affiliations:
1 Observatoire de la Côte d’Azur, CNRS, B.P. 4229, 06304 Nice Cedex 4, France
Phys. Plasmas 14, 082502 (2007)
/content/aip/journal/pop/14/8/10.1063/1.2751601
http://aip.metastore.ingenta.com/content/aip/journal/pop/14/8/10.1063/1.2751601
View: Figures

## Figures

FIG. 1.

Comparison between the imaginary part of the function (thin solid line) with the corresponding Padé approximants (crosses) and (thick dashed line). The inset displays the same quantities in a smaller range of , close to the origin.

FIG. 2.

Normalized frequency (left) and damping rate (right) vs , for KAWs with , , and (top), (middle), and (bottom). Here and in the following figures, the solid line refer to the full kinetic theory and the crosses to the prediction of the model when using the Padé approximant; The crosses in the top panels are obtained with the Padé approximant.

FIG. 3.

Normalized frequency (left) and damping rate (right) vs , for KAWs with , , and for (top), (middle), and (bottom).

FIG. 4.

Normalized frequency (left) and damping rate (right) vs , for KAWs with , for (top) and (bottom).

FIG. 5.

Normalized frequency (left) and damping rate (right) vs , for AWs with , , and (top) and (bottom).

FIG. 6.

Normalized frequency (left) and damping rate (right), where is the sound velocity, vs , for quasi-transverse slow waves with , and (top) and (bottom).

FIG. 7.

Normalized frequency (left) and damping rate (right) vs for quasi-transverse slow waves with , and (top) and (bottom).

FIG. 8.

Normalized frequency (left) and damping rate (right) vs for fast waves with , , and .

FIG. 9.

Normalized frequency (left) and damping rate (right) vs , for fast waves with , , and (top), (middle), and (bottom).

FIG. 10.

Normalized growth rate vs for mirror modes with , , , , and (top, left) and , , , and (top, right) as a function of . Same for , , , , and (bottom, left). and (bottom, right).

/content/aip/journal/pop/14/8/10.1063/1.2751601
2007-08-16
2014-04-16

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