Abstract

Abstract. Recently, it has been established that interplanetary coronal mass ejections (ICMEs) can dramatically affect both trapped electron fluxes in the outer radiation belt and precipitating electron fluxes lost from the belt into the atmosphere. Precipitating electron fluxes and energies can vary over a range of timescales during these events. These variations depend on the initial energy and location of the electron population and the ICME characteristics and structures. One important factor controlling electron dynamics is the magnetic field orientation within the ejecta that is an integral part of the ICME. In this study, we examine Van Allen Probes (RBSPs) and Polar Orbiting Environmental Satellites (POESs) data to explore trapped and precipitating electron fluxes during two ICMEs. The ejecta in the selected ICMEs have magnetic cloud characteristics that exhibit the opposite sense of the rotation of the north–south magnetic field component (BZ). RBSP data are used to study trapped electron fluxes in situ, while POES data are used for electron fluxes precipitating into the upper atmosphere. The trapped and precipitating electron fluxes are qualitatively analysed to understand their variation in relation to each other and to the magnetic cloud rotation during these events. Inner magnetospheric wave activity was also estimated using RBSP and Geostationary Operational Environmental Satellite (GOES) data. In each event, the largest changes in the location and magnitude of both the trapped and precipitating electron fluxes occurred during the southward portion of the magnetic cloud. Significant changes also occurred during the end of the sheath and at the sheath–ejecta boundary for the cloud with south to north magnetic field rotation, while the ICME with north to south rotation had significant changes at the end boundary of the cloud. The sense of rotation of BZ and its profile also clearly affects the coherence of the trapped and/or precipitating flux changes, timing of variations with respect to the ICME structures, and flux magnitude of different electron populations. The differing electron responses could therefore imply partly different dominant acceleration mechanisms acting on the outer radiation belt electron populations as a result of opposite magnetic cloud rotation.

Highlights

  • The Van Allen radiation belts are highly dynamic regions of charged particles trapped in the Earth’s geomagnetic field (Van Allen, 1981)

  • ultra-low frequency (ULF)– Pc5 wave power weakens during the time period of the northward portion of the ejecta but stays at relatively enhanced levels that persist for a few hours after the ejecta trailing edge, while Electromagnetic ion cyclotron (EMIC) power decreases to pre-event levels

  • We have studied the electron response to two different interplanetary coronal mass ejections (ICMEs) events here, examining fluxes that precipitate into the upper atmosphere and fluxes trapped in the outer radiation belt

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Summary

Introduction

The Van Allen radiation belts are highly dynamic regions of charged particles trapped in the Earth’s geomagnetic field (Van Allen, 1981). The variation of the trapped flux of electrons in the outer radiation belt and the subsequent precipitation into the upper atmosphere is extremely complex due to the wide range of processes acting on the various electron populations. The Van Allen Probes measure trapped electron fluxes within the radiation belts while POES provides a measure of the electron fluxes precipitating into the upper atmosphere We use these data to qualitatively analyse the relationship between trapped outer radiation belt electron fluxes, from source to ultrarelativistic energies, and precipitating fluxes during these two ICMEs. Of particular interest is the electron response to different magnetic field orientations within each event and to opposite magnetic cloud rotations in the two case studies

Data and methods
30 December 2015–2 January 2016
26–30 June 2013
Electron flux and precipitation
Discussion
Summary
Full Text
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