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dc.contributor.authorVoitcu, G.
dc.contributor.authorEchim, M.
dc.date2018
dc.date.accessioned2018-11-15T20:12:53Z
dc.date.available2018-11-15T20:12:53Z
dc.identifier.urihttps://orfeo.belnet.be/handle/internal/7141
dc.descriptionIn 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 "measured" by a virtual satellite launched into the simulation domain.
dc.languageeng
dc.titleCrescent-shaped electron velocity distribution functions formed at the edges of plasma jets interacting with a tangential discontinuity
dc.typeArticle
dc.subject.frascatiPhysical sciences
dc.audienceScientific
dc.source.titleAnnales Geophysicae
dc.source.volume36
dc.source.issue6
dc.source.page1521-1535
Orfeo.peerreviewedYes
dc.identifier.doi10.5194/angeo-36-1521-2018


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