HR: 0800h
AN: SM51A-07 [Abstracts]
TI: Kinetic Simulations of Collisionless Reconnection in Pair Plasmas
AU: * Yin, L
EM: lyin@lanl.gov
AF: Los Alamos National Laboratory, MS-F699, Los Alamos, NM 87545, United States
AU: Daughton, W
EM: william-daughton@uiowa.edu
AF: University of Iowa, Department of Physics & Astronomy, 511 VAN, Iowa City, IA 52242,
United States
AU: Bowers, K J
EM: kevin.j.bowers@ieee.org
AF: Los Alamos National Laboratory, MS-F699, Los Alamos, NM 87545, United States
AB:
Despite a great deal of research effort, many basic issues regarding
collisionless reconnection remain poorly understood. Although fully
kinetic simulations offer a first principles approach, the large
separation between electron and ion spatial and temporal scales has
severally limited these computational studies. In contrast, the problem
of magnetic reconnection in an electron-positron plasma is feasible in
both 2D and 3D. It has been suggested that reconnection in pair plasmas
may be of interest to certain astrophysical problems. Furthermore, this
limit is useful to consider in the effort to understand the essential
physics of magnetic reconnection, since there is no scale separation
and it can be shown analytically that there are no whistler waves.
In this work, we first examine the limit of large-scale 2D systems.
Consistent with recent publications, it is demonstrated that reconnection
rates remain fast for very large systems but a steady-state is never
achieved. Instead the reconnection dynamics proceeds by the repeated
formation of secondary islands as the diffusion region expands.
From linear Vlasov theory, the unstable eigenmodes in a pair plasma
include collisionless tearing and the drift-kink mode. In 3D simulations,
the box length in the direction of the current can be selected to either
permit or exclude the drift-kink. In the limit where the box length is
short enough to exclude the drift-kink mode, reconnection proceeds
essentially in the same manner as the 2D simulations. However, when the
simulation box is long enough to allow the drift-kink mode, the reconnection
dynamics change dramatically with complicated 3D structures resulting from
the nonlinear interaction between collisionless tearing and drift-kink.
These results may have some relevance to reconnection in hydrogen plasmas
since the drift-kink mode is replaced by the ion-ion kink mode at high
mass ratio.
DE: 7526 Magnetic reconnection (2723, 7835)
DE: 7835 Magnetic reconnection (2723, 7526)
SC: SPA-Magnetospheric Physics [SM]
MN: 2007 Joint Assembly