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磁重联中电子扩散区的机制。

Regimes of the electron diffusion region in magnetic reconnection.

机构信息

Department of Physics, Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.

出版信息

Phys Rev Lett. 2013 Mar 29;110(13):135004. doi: 10.1103/PhysRevLett.110.135004. Epub 2013 Mar 28.

Abstract

The electron diffusion region during magnetic reconnection lies in different regimes depending on the pressure anisotropy, which is regulated by the properties of thermal electron orbits. In kinetic simulations at the weakest guide fields, pitch angle mixing in velocity space causes the outflow electron pressure to become nearly isotropic. Above a threshold guide field that depends on a range of parameters, including the normalized electron pressure and the ion-to-electron mass ratio, electron pressure anisotropy develops in the exhaust and supports extended current layers. This new regime with electron current sheets extending to the system size is also reproduced by fluid simulations with an anisotropic closure for the electron pressure. It offers an explanation for recent spacecraft observations.

摘要

在磁重联过程中,电子扩散区处于不同的状态,这取决于压力各向异性,而压力各向异性由热电子轨道的性质决定。在最弱引导场的动力学模拟中,速度空间中的进动混合导致流出电子压力几乎各向同性。在一个取决于一系列参数的阈值引导场以上,包括归一化电子压力和离子与电子的质量比,在尾流中会产生电子压力各向异性,并支持扩展电流层。具有各向异性电子压力封闭的流体模拟也再现了这种新的状态,其中电子电流片延伸到系统尺寸。这为最近的航天器观测提供了一种解释。

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