|
Read Full Article (file size: 609663 bytes) Cited by
JOURNAL OF GEOPHYSICAL RESEARCH,
VOL. 107, NO. A8,
1183,
doi:10.1029/2001JA009229,
2002
Total electron and proton energy input during auroral substorms: Remote sensing with IMAGE-FUV
B. Hubert
Laboratoire de Physique Atmosphérique et Planétaire,
Université de Liège,
Liège-Ougrée,
Belgium
J.-C. Gérard
Laboratoire de Physique Atmosphérique et Planétaire,
Université de Liège,
Liège-Ougrée,
Belgium
D. S. Evans
NOAA Space Environment Center,
Boulder,
Colorado,
USA
M. Meurant
Laboratoire de Physique Atmosphérique et Planétaire,
Université de Liège,
Liège-Ougrée,
Belgium
S. B. Mende
Space Sciences Laboratory,
University of California,
Berkeley,
California,
USA
H. U. Frey
Space Sciences Laboratory,
University of California,
Berkeley,
California,
USA
T. J. Immel
Space Sciences Laboratory,
University of California,
Berkeley,
California,
USA
Abstract
The IMAGE satellite carries three FUV imagers observing N2 LBH, O I 1356 Å, and HI Lyman α emissions in the polar aurora. These simultaneous observations are used to characterize the
precipitating electron and proton energy fluxes. The proton energy flux is derived from the Lyman α measurements on the basis
of efficiency curves calculated with a Monte Carlo simulation of the proton aurora. The resulting proton contribution to the
N2 LBH and O I 1356 Å emissions is calculated and subtracted to obtain the electron contribution in the other two channels.
These two quantities are used to determine the precipitating electron average energy and energy flux. The proton and electron
energy fluxes are integrated over the hemisphere to obtain the rate of auroral energy dissipation (hemispheric power) carried
by the protons and electrons separately. The time development of the proton and electron aurora during four winter time events
is examined. Although the onsets of the proton and electron aurora coincide in time and space, the time of the peak of energy
dissipation and the recovery time are often found to differ. The fractional energy flux carried by the protons is highest
during quiet periods and reaches a minimum during the most active phase of the substorms. This result is in agreement with
the dependence of the fractional proton hemispheric power on magnetic activity measured by NOAA 15. The hemispheric power
deduced from the FUV images is compared to the NOAA-deduced values and found to be in reasonable agreement. Sources of uncertainties
in the determination of the hemispheric power are discussed on the basis of several sensitivity tests. In particular, it is
found that the most critical factor is the assumption made on the energy of the auroral protons if this energy is <25 keV.
Published 14
August
2002.
Index Terms: 0358 Atmospheric Composition and Structure: Thermosphere—energy deposition; 0310 Atmospheric Composition and Structure: Airglow and aurora; 2716 Magnetospheric Physics: Energetic particles, precipitating; 2788 Magnetospheric Physics: Storms and substorms.
Read Full Article (file size: 609663 bytes) Cited by
Citation: Hubert, B., J.-C. Gérard, D. S. Evans, M. Meurant, S. B. Mende, H. U. Frey, and T. J. Immel
(2002),
Total electron and proton energy input during auroral substorms: Remote sensing with IMAGE-FUV,
J. Geophys. Res.,
107(A8),
1183,
doi:10.1029/2001JA009229.
Copyright 2002 by the American Geophysical Union.
|