|
Read Full Article (file size: 2374602 bytes) Cited by
JOURNAL OF GEOPHYSICAL RESEARCH,
VOL. 111,
A03208,
doi:10.1029/2005JA011469,
2006
Origin of geosynchronous relativistic electron events
H.-J. Kim
Department of Astronomy and Space Science, College of Natural Sciences and Institute for Basic Science Research, Chungbuk
National University, Chungbuk, Korea
K. C. Kim
Department of Astronomy and Space Science, College of Natural Sciences and Institute for Basic Science Research, Chungbuk
National University, Chungbuk, Korea
D.-Y. Lee
Department of Astronomy and Space Science, College of Natural Sciences and Institute for Basic Science Research, Chungbuk
National University, Chungbuk, Korea
Gordon Rostoker
Department of Physics, University of Alberta, Edmonton, Alberta, Canada
Abstract
We have investigated the characteristics of solar wind and magnetospheric conditions associated with the occurrence of geosynchronous
relativistic electron events. Most of the geosynchronous relativistic events for April 1999 to December 2002 are found to
occur during prolonged (a number of days) quiet intervals following the appearance of high-speed solar wind streams. In a
typical relativistic event, the electron fluxes begin to increase by orders of magnitude when the solar wind density drops
after reaching a sharp peak at the leading edge of a high-speed stream. The increased fluxes stay at a high level until the
quiet solar wind conditions cease. In addition, enhanced ULF wave activity and substorm injections of 10s to 100s keV electrons
are observed at the time of the large flux increases in the events. We found that geosynchronous relativistic events can be
observed only when both the solar wind and magnetospheric wave/substorm injection conditions are favorable regardless of whether
or not a magnetic storm takes place. These observations suggest the following scenario for the occurrence of a geosynchronous
relativistic electron event: (1) Quiet solar wind conditions (i.e., no strong solar wind pressure and large southward turnings
of IMF Bz) can lead to stable and more dipole-like magnetospheric configurations in which the geosynchronous orbit is located well
inside the trapping boundary of the energetic electrons. (2) If a large population of MeV electrons is generated (by some
acceleration process(es) involving enhanced ULF wave and substorm injections) in the inner magnetosphere, it can be trapped
and effectively accumulated to a high intensity. (3) The high electron flux can persist for a number of days in the geosynchronous
region as long as the solar wind conditions remain quiescent. The occurrence of a geosynchronous relativistic electron event
requires not only the proper acceleration process and sufficient seed electrons but also no significant loss process that
dominates over any acceleration/source.
Received 11
October
2005;
accepted 28
November
2005;
published 10
March
2006.
Keywords: relativistic electron events;
geosynchronous;
magnetic storms;
electron loss and acceleration.
Index Terms: 2720 Magnetospheric Physics: Energetic particles: trapped; 2774 Magnetospheric Physics: Radiation belts; 2784 Magnetospheric Physics: Solar wind/magnetosphere interactions; 2740 Magnetospheric Physics: Magnetospheric configuration and dynamics; 7984 Space Weather: Space radiation environment.
Read Full Article (file size: 2374602 bytes) Cited by
Citation: Kim, H.-J., K. C. Kim, D.-Y. Lee, and G. Rostoker
(2006),
Origin of geosynchronous relativistic electron events,
J. Geophys. Res.,
111,
A03208,
doi:10.1029/2005JA011469.
Copyright 2006 by the American Geophysical Union.
|