HR: 1400h
AN: SM33B-02 [Abstracts]
TI: Modeling pitch-angle and gyrophase restricted ~0.5~MeV foreshock ions
AU: * Wilber, M
EM: wilber@ssl.berkeley.edu
AF: U. California, 7 Gauss Way, Space Sciences Laboratory, Berkeley, CA 94720, United States
AU: Meziane, K
EM: karim@unb.ca
AF: U. New Brunswick, Department of Physics, Fredericton, CA , United States
AU: Liin, R P
EM: rlin@ssl.berkeley.edu
AF: U. California, 7 Gauss Way, Space Sciences Laboratory, Berkeley, CA 94720, United States
AU: Parks, G K
EM: parks@ssl.berkeley.edu
AF: U. California, 7 Gauss Way, Space Sciences Laboratory, Berkeley, CA 94720, United States
AB:
Ions with energies > 100~keV backstreaming from the bow shock have been well-studied, with most observed
fitting into three catagories: those with isotropic distributions accelerated via diffusive processes, typically having
energies no greater than 250 keV; those with pitch angle, and sometimes gyrophase, constrained distributions
extending past 1 MeV in energy, accelerated during single encounters with the shock via the shock drift
mechanism; and those of magnetospheric origin that `leak' across the magnetopasue and find their way to the
upstream. In principle, some of these mechanisms could act in concert, although that has not been examined
thoroughly. We have examined relatively infrequent Wind/3DP observations that appear to be of the second type
(restricted in pitch angle and gyrophase), but which have no apparent source of seed particles needed to produce
the observed fluxes using straightforward application of shock drift acceleration theory. Due to the different travel
times required for ions of different pitch angles and energies to travel from the shock to the spacecraft, and
gyrophase dependent trajectories for ions with gyroradii of the order of an Earth radius, a single distribution
snapshot is a convolution of sources that can be well-distributed along the bow shock. In order to better
understand our observations we have applied particle tracking methods to find how ions at different energies and
arrival directions map back to the shock, which permits us to model point-by-point contributions to the
distributions observed at the spacecraft. We present results from this investigation, and consider different
hypotheses for producing the unobserved, but required, seed populations.
DE: 2114 Energetic particles (7514)
DE: 2154 Planetary bow shocks
DE: 2451 Particle acceleration
DE: 7807 Charged particle motion and acceleration
SC: SPA-Magnetospheric Physics [SM]
MN: 2007 Joint Assembly