l = 1 Diocotron Instability of Single Charged Plasmas1
A. V. Arefiev*, I. A. Kotelnikov**, M. Romé***, and R. Pozzoli***
*University of Texas at Austin, Austin, TX, USA
**Budker Institute of Nuclear Physics, Siberian Division, Russian Academy of Sciences,
pr. Akademika Lavrenteva 11, Novosibirsk, 630090 Russia
e-mail: Kotelnikov@inp.nsk.su
***Istituto Nazionale di Fisica della Materia, U.d.R. Milano, and Dipartimento di Fisica,
Università degli Studi di Milano, Italy
e-mail: Massimiliano.Rome@mi.infn.it; e-mail: Roberto.Pozzoli@mi.infn.it
Received August 24, 2001
AbstractThe linear stability analysis of the l = 1 diocotron perturbations in a low density single charged
plasma confined in a cylindrical Penning trap is critically revisited. Particular attention is devoted to the insta-
bility due to the presence of one or more stationary points in the radial profile of the azimuthal rotation fre-
quency. The asymptotic analysis of Smith and Rosenbluth for the case of a single-bounded plasma column
(algebraic instability proportional to t 1/2) is generalized in a few respects. In particular, the existence of unper-
turbed density profiles that give rise to l = 1 algebraic instabilities growing with time proportionally to t 1
1/m,
m
3 being the order of a stationary point in the rotation frequency profile, and even proportionally to t, is
pointed out. It is also shown that smoothing the density jumps of a multistep density profile can convert alge-
braically growing perturbations into exponentially decaying modes. The relevant damping rates are computed.
The asymptotic analysis (t
) of the fundamental diocotron perturbations is then generalized to the case
of a cylindrical Penning trap with an additional coaxial inner conductor. It is shown that the algebraic instability
found in the case of a single-bounded plasma column becomes exponential at longer times. The relevant linear
growth rate is computed by a suitable inverse Laplace transform (contour integral in the complex plane). In the
particular case of an uncharged inner conductor of radius a, the growth rate is shown to scale as a 4/3 for a
0.
The theoretical results are compared with the numerical solution of the linearized two-dimensional drift Poisson
equations. © 2002 MAIK Nauka/Interperiodica.
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