Three‐dimensional Electron‐scale Magnetic Reconnection in Earth's Magnetosphere

Author(s):  
Z. H. Zhong ◽  
M. Zhou ◽  
X. H. Deng ◽  
L. J. Song ◽  
D. B. Graham ◽  
...  
2011 ◽  
Vol 38 (20) ◽  
pp. n/a-n/a ◽  
Author(s):  
M. Oka ◽  
T.-D. Phan ◽  
J. P. Eastwood ◽  
V. Angelopoulos ◽  
N. A. Murphy ◽  
...  

2021 ◽  
Author(s):  
S. Toledo‐Redondo ◽  
M. André ◽  
N. Aunai ◽  
C. R. Chappell ◽  
J. Dargent ◽  
...  

2009 ◽  
Vol 16 (1) ◽  
pp. 1-10 ◽  
Author(s):  
F. Califano ◽  
M. Faganello ◽  
F. Pegoraro ◽  
F. Valentini

Abstract. The Earth's magnetosphere and solar wind environment is a laboratory of excellence for the study of the physics of collisionless magnetic reconnection. At low latitude magnetopause, magnetic reconnection develops as a secondary instability due to the stretching of magnetic field lines advected by large scale Kelvin-Helmholtz vortices. In particular, reconnection takes place in the sheared magnetic layer that forms between adjacent vortices during vortex pairing. The process generates magnetic islands with typical size of the order of the ion inertial length, much smaller than the MHD scale of the vortices and much larger than the electron inertial length. The process of reconnection and island formation sets up spontaneously, without any need for special boundary conditions or initial conditions, and independently of the initial in-plane magnetic field topology, whether homogeneous or sheared.


2017 ◽  
Vol 83 (6) ◽  
Author(s):  
Matteo Faganello ◽  
Francesco Califano

The Kelvin–Helmholtz instability, proposed a long time ago for its role in and impact on the transport properties at magnetospheric flanks, has been widely investigated in the Earth’s magnetosphere context. This review covers more than fifty years of theoretical and numerical efforts in investigating the evolution of Kelvin–Helmholtz vortices and how the rich nonlinear dynamics they drive allow solar wind plasma bubbles to enter into the magnetosphere. Special care is devoted to pointing out the main advantages and weak points of the different plasma models that can be adopted for describing the collisionless magnetospheric medium and in underlying the important role of the three-dimensional geometry of the system.


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