Drift instabilities

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This is a page under constuction. It is possible that the author have gotten stuck, or are merely in the process of completing the article and it's supports. It is also possible that what is written is not in fact rigorous, and thus should be treated with lessened credibility. Beware! If possible, help out!

[1] N.A. Krall, Advances in Plasma Physics, Vol. 1. (1968) 153.

[2] Krall & Trivelpiece, p.430 ff.

[3] Hinton & Hazeltine. Rev. of Modern Physics 48 (1976) 239.

[4] A.B. Mikhailovskii, Theory of Plasma Instabilities , Vol II, (1974) (Discusses both fluid and kinetic derivations).

[5] Coppi, Rosenbluth, Sagdeev, Phys. Fluids. 10, 582 (1967).

[6] Pearlstein & Berk, Phys. Rev. Lett. 23 (1969) 220 ("Universal Mode")

[7] Coppi, Rosenbluth & Sagdeev, Phys. Fluids 10 (1967) 582.

[8] Hahm, Tang, Phys. Fluids B 1 (1989) 1185. (ηi-mode with Resonances, (etai)cit analysis)

The toriodal geometry changes the basic mode structure to "balloning-type" character alone the field line.

    • \nabla \mathbf{B} drift effects strong.
  • Trapped particle dynmaics appear. (Trapped ηi ion modes).

[9] Guzdan et. al. Phys. Fluids. 26. 673 (1983)

[10] Hurton, et. al. Phys. Fluids. 24. 1077 (1987).

[11] Tang, Rewoldt, Chen, P.F. 29, 3715 (1987).

[12] Biglan, et. al. P. F. B. 1, 109 (1989).

[13] Romanelli, P. F. B. 1. (1989)

[14] Guo, et. al, Plasma Phys, 31, 423 (1989) (Possible local q dependence).

This page was recovered in October 2009 from the Plasmagicians page on Drift_instabilities dated 20:39, 15 May 2007.

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