Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity

<p>In this paper we discuss numerical simulations that illustrate a physical mechanism leading to the formation of crescent-shaped electron velocity distribution functions at the edges of a high-speed plasma jet impacting on a thin, steep and impenetrable tangential discontinuity with no ma...

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Main Authors: G. Voitcu, M. Echim
Format: Article
Language:English
Published: Copernicus Publications 2018-11-01
Series:Annales Geophysicae
Online Access:https://www.ann-geophys.net/36/1521/2018/angeo-36-1521-2018.pdf
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spelling doaj-82dfaa73649b42a69cc4757bb11a51832020-11-25T00:17:05ZengCopernicus PublicationsAnnales Geophysicae0992-76891432-05762018-11-01361521153510.5194/angeo-36-1521-2018Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuityG. Voitcu0M. Echim1M. Echim2Institute of Space Science, Magurele, 077125, RomaniaInstitute of Space Science, Magurele, 077125, RomaniaBelgian Institute of Space Aeronomy, Brussels, 1180, Belgium<p>In this paper we discuss numerical simulations that illustrate a physical mechanism leading to the formation of crescent-shaped electron velocity distribution functions at the edges of a high-speed plasma jet impacting on a thin, steep and impenetrable tangential discontinuity with no magnetic shear. We use three-dimensional particle-in-cell simulations to compute the velocity distribution function of electrons in different areas of the plasma jet and at different phases of the interaction with the discontinuity. The simulation set-up corresponds to an idealized, yet relevant, magnetic configuration likely to be observed at the frontside magnetopause under the northward interplanetary magnetic field. The combined effect of the gradient-B drift and the remote sensing of large Larmor radius electrons leads to the formation of crescent-shaped electron velocity distribution functions. We provide examples of such distributions <q>measured</q> by a virtual satellite launched into the simulation domain.</p>https://www.ann-geophys.net/36/1521/2018/angeo-36-1521-2018.pdf
collection DOAJ
language English
format Article
sources DOAJ
author G. Voitcu
M. Echim
M. Echim
spellingShingle G. Voitcu
M. Echim
M. Echim
Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity
Annales Geophysicae
author_facet G. Voitcu
M. Echim
M. Echim
author_sort G. Voitcu
title Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity
title_short Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity
title_full Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity
title_fullStr Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity
title_full_unstemmed Crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity
title_sort crescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity
publisher Copernicus Publications
series Annales Geophysicae
issn 0992-7689
1432-0576
publishDate 2018-11-01
description <p>In this paper we discuss numerical simulations that illustrate a physical mechanism leading to the formation of crescent-shaped electron velocity distribution functions at the edges of a high-speed plasma jet impacting on a thin, steep and impenetrable tangential discontinuity with no magnetic shear. We use three-dimensional particle-in-cell simulations to compute the velocity distribution function of electrons in different areas of the plasma jet and at different phases of the interaction with the discontinuity. The simulation set-up corresponds to an idealized, yet relevant, magnetic configuration likely to be observed at the frontside magnetopause under the northward interplanetary magnetic field. The combined effect of the gradient-B drift and the remote sensing of large Larmor radius electrons leads to the formation of crescent-shaped electron velocity distribution functions. We provide examples of such distributions <q>measured</q> by a virtual satellite launched into the simulation domain.</p>
url https://www.ann-geophys.net/36/1521/2018/angeo-36-1521-2018.pdf
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