M. Hirahara et al., 2 TYPES OF ION ENERGY DISPERSIONS OBSERVED IN THE NIGHTSIDE AURORAL REGIONS DURING GEOMAGNETICALLY DISTURBED PERIODS, J GEO R-S P, 101(A4), 1996, pp. 7749-7767
The Akebono satellite has observed two types of energy dispersion sign
atures of discrete ion precipitation event in the nightside auroral re
gions during active geomagnetic conditions. The charged particle exper
iments and electric and magnetic field detectors on board Akebono prov
ide us with essential clues to characterize the source regions and acc
eleration and/or injection processes associated with these two types o
f ion. signatures. The magnetic field data obtained simultaneously by
the geosynchronous GOES 6 and 7 satellites and the ground magnetograms
are useful to examine their relationships with geomagnetic activity.
Mass composition data and pitch angle distributions show that differen
t sources and processes should be attributed to two types (Types I and
II) of energy dispersion phenomena, Type I consists of multiple bounc
ing ion clusters constituted by H+. These H+ clusters tend to be detec
ted at the expansion phase of substorms and have characteristic multip
le energy-dispersed signatures. Type II consists of O+ energy dispersi
on(s), which is often observed at the recovery phase. It is reasonable
to consider that the H+ clusters of Type I are accelerated by dipolar
ization at the equator, are injected in the field-aligned direction, a
nd bounce on closed field lines after the substorm onset. We interpret
these multiple energy dispersion events as mainly due to the time-of-
flight (TOF) effect, although the convection may influence the energy-
dispersed traces. Based on the TOF model, we estimate the source dista
nce to be 20-30 R(E) along the field lines. On the other hand, the Oenergy dispersion of Type II is a consequence of reprecipitation of te
rrestrial ions ejected as an upward flowing ion (UFI) beam from the up
per ionosphere by a parallel electrostatic potential difference. The O
+ energy dispersion is induced by the E x B drift during the field-ali
gned transport from the source region to the observation point.