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Titel On background density dependence of non-stationary collisionless magnetic reconnection.
VerfasserIn Andrey Divin, Yuri Khotyaintsev, Andris Vaivads, Mats André, Giovanni Lapenta, Stefano Markidis, Vyacheslav Olshevsky
Konferenz EGU General Assembly 2014
Medientyp Artikel
Sprache Englisch
Digitales Dokument PDF
Erschienen In: GRA - Volume 16 (2014)
Datensatznummer 250098511
Publikation (Nr.) Volltext-Dokument vorhandenEGU/EGU2014-14193.pdf
 
Zusammenfassung
Even the simplest 2D configuration susceptible to magnetic reconnection (namely, Harris current sheet), possesses a number of "free parameters" that determine the dynamics and energetics of the process. Among such parameters are Ti-ˆ•Te ratio, guide field value, current sheet thickness, etc. In this presentation we systematically study the effect of changing the background density (from nb-ˆ•n0 = 0.5 to nb-ˆ•n0 = 0.003), which covers the range of lobe density values observed in the Earth’s magnetotail. Two-dimensional Particle-in-Cell (PIC) simulations are performed using implicit parallel code iPIC3D with double-periodic configuration. Increase of the jet front magnetic field (Bz) with nb decrease is in agreement with simulations by [Wu 2012]. The elevated Bz region is several times larger (in the Z direction) than the initial current layer thickness, whereas large normal electric field (Ex) area is focused between the front and current sheet edge. Normal electric field has a bipolar profile (in the X direction), intensity scales roughly as (nb-ˆ•n0)-1-ˆ•2 with changing nb. Intense waves are generated at magnetic reconnection separatrices in the low density case. The waves can be excited either by separatrix electron flow disruption or by EH propagation. We conclude that the ’standard’ picture of GEM-type reconnection is retained for various nb-ˆ•n0 ratios in two-dimensional configurations, with minor quantitative differences attributed to steeper front shape and faster propagation at low nb densities.