Equilibrium and Stability of Asymmetric Plasmas

Asymmetric Plasmas

When azimuthally-asymmetric potentials are applied to the wall of a Penning-Malmberg trap, the plasma deform into a stationary cylinder of noncircular cross-section. Such highly deformed, stationary non-neutral plasma columns are unexpectedly long-lived. Normally, non-neutral plasmas are stored in Penning-Malmberg traps with cylindrically-symmetric wall boundary potentials, and the equilibrium plasma shape is a symmetric cylinder. Wall potentials can be applied by biasing isolated sections of the wall surrounding the plasma.



A typical deformed shape, found experimentally is shown below.



Since the wall potentials are no longer symmetric, angular momentum conservation is no longer guaranteed, and the standard justification for the long lifetime of non-neutral plasmas is no longer applicable. Consequently, the long lifetimes of these deformed plasmas was a surprise.

Theoretical study of these deformed plasmas begins with understanding the equilibrium conditions. Chu et. al. studied the equilibrium shapes of the slightly deformed plasmas that result from small wall potential perturbations. The results of Chu’s analytic (left) and numeric (center) models for the experimental plasma at the right are shown below:




Recently we have been studying highly deformed plasmas such as the one below. In principle, and shape even one as deformed as the one below, can be put in equilibrium



Proving that all shapes can be put into equilibrium turns out to be a new problem in Poisson theory.

All deformed plasmas can be put in equilibria, but not all deformed plasmas are in stable equilibria. When the deformation is small, the plasma is in a maximal energy state. Maximal energy states (like a ball at the top of a mountain) are normally thought to be unstable. But in our system, potential energy cannot be turned in kinetic energy, so a maximal energy state is actually stable. Hence the plasma are typically in stable equilibria. But if the plasma is deformed to much, the stability will bifurcate. For example, the movie below shows the effect of applying an ever greater cos(2q) wall potentials to an experimental plasma.  Click on the plasma to get a more informative movie. Determining the stability of more complicated shapes is a difficult problem in advanced bifurcation theory.  The symmetry of the system has a strong influence on the type of bifurcation, and many high order bifurcations are predicted to occur.