The nightside magnetic field line open–closed boundary and polar rain electron energy-latitude dispersion

The polar rain electrons near the open–closed field line boundary on the nightside often exhibit energy-latitude dispersion, in which the energy decreases with decreasing latitude. The solar wind electrons from the last open-field line would <i><b>E</b></i> &times; <...

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Main Authors: S. Wing, Y. L. Zhang
Format: Article
Language:English
Published: Copernicus Publications 2015-01-01
Series:Annales Geophysicae
Online Access:https://www.ann-geophys.net/33/39/2015/angeo-33-39-2015.pdf
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spelling doaj-629e958eff334567b332c729dd764cd82020-11-25T00:29:15ZengCopernicus PublicationsAnnales Geophysicae0992-76891432-05762015-01-0133394610.5194/angeo-33-39-2015The nightside magnetic field line open–closed boundary and polar rain electron energy-latitude dispersionS. Wing0Y. L. Zhang1The Johns Hopkins University Applied Physics Laboratory, Laurel, Maryland, USAThe Johns Hopkins University Applied Physics Laboratory, Laurel, Maryland, USAThe polar rain electrons near the open–closed field line boundary on the nightside often exhibit energy-latitude dispersion, in which the energy decreases with decreasing latitude. The solar wind electrons from the last open-field line would <i><b>E</b></i> &times; <i><b>B</i></b> drift equatorward as they move toward the ionosphere, resulting in the observed dispersion. This process is modeled successfully by an open-field line particle precipitation model. The existing method for determining the magnetotail <i>X</i> line distance from the electron dispersion underestimates the electron path length from the <i>X</i> line to the ionosphere by at least 33%. The best estimate of the path length comes from using the two highest energy electrons in the dispersion region. The magnetic field line open–closed boundary is located poleward of the highest energy electrons in the dispersion region, which in turn is located poleward of Defense Meteorological Satellite Program (DMSP) b6, b5e, and b5i boundaries. In the four events examined, b6 is located at least 0.7–1.5° equatorward of the magnetic field line open–closed boundary. The energy-latitude dispersion seen in the electron overhang may result from the plasma sheet electron curvature and gradient drifts into the newly closed field line.https://www.ann-geophys.net/33/39/2015/angeo-33-39-2015.pdf
collection DOAJ
language English
format Article
sources DOAJ
author S. Wing
Y. L. Zhang
spellingShingle S. Wing
Y. L. Zhang
The nightside magnetic field line open–closed boundary and polar rain electron energy-latitude dispersion
Annales Geophysicae
author_facet S. Wing
Y. L. Zhang
author_sort S. Wing
title The nightside magnetic field line open–closed boundary and polar rain electron energy-latitude dispersion
title_short The nightside magnetic field line open–closed boundary and polar rain electron energy-latitude dispersion
title_full The nightside magnetic field line open–closed boundary and polar rain electron energy-latitude dispersion
title_fullStr The nightside magnetic field line open–closed boundary and polar rain electron energy-latitude dispersion
title_full_unstemmed The nightside magnetic field line open–closed boundary and polar rain electron energy-latitude dispersion
title_sort nightside magnetic field line open–closed boundary and polar rain electron energy-latitude dispersion
publisher Copernicus Publications
series Annales Geophysicae
issn 0992-7689
1432-0576
publishDate 2015-01-01
description The polar rain electrons near the open–closed field line boundary on the nightside often exhibit energy-latitude dispersion, in which the energy decreases with decreasing latitude. The solar wind electrons from the last open-field line would <i><b>E</b></i> &times; <i><b>B</i></b> drift equatorward as they move toward the ionosphere, resulting in the observed dispersion. This process is modeled successfully by an open-field line particle precipitation model. The existing method for determining the magnetotail <i>X</i> line distance from the electron dispersion underestimates the electron path length from the <i>X</i> line to the ionosphere by at least 33%. The best estimate of the path length comes from using the two highest energy electrons in the dispersion region. The magnetic field line open–closed boundary is located poleward of the highest energy electrons in the dispersion region, which in turn is located poleward of Defense Meteorological Satellite Program (DMSP) b6, b5e, and b5i boundaries. In the four events examined, b6 is located at least 0.7–1.5° equatorward of the magnetic field line open–closed boundary. The energy-latitude dispersion seen in the electron overhang may result from the plasma sheet electron curvature and gradient drifts into the newly closed field line.
url https://www.ann-geophys.net/33/39/2015/angeo-33-39-2015.pdf
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