反常跨场扩散对场向电流产生的影响

Takashi Yamamoto, S. Inoue, C. Meng
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引用次数: 6

摘要

首先,基于对极光磁层宽带静电噪声和阿尔芬波噪声的卫星观测,在准线性理论的框架内,我们表明质子(异常交叉场)扩散系数在通量管上的平均至少在扰动期可能达到玻姆率的显著部分。其次,作为最近提出的磁层热等离子体环面(HPT)在双涡旋胞体对流的影响下(当行星际磁场(IMF)向南时)“自然畸变”可产生一对1区和2区场向电流(FACs)模型的扩展,我们研究了异常跨场扩散对由HPT极化引起的大规模场向电流可能产生的影响。在磁层中,热(≥1 keV)等离子体粒子主要分布在一个磁壳中,该磁壳与南北两极电离层上两个椭圆形的弥散极光相连。这样的热等离子体群被称为热等离子体环面(HPT)。数值计算特别表明,这种影响对FAC型的主要改变是在午夜扇区出现三重FAC结构(即向上的FAC区夹在两个向下的FAC区之间),至少在亚风暴期间可以从卫星观测中识别出来。作为这种三重FAC结构形成的直接结果,哈朗不连续出现在电位图中。因此,哈朗不连续的形成可以理解为磁漂移和异常交叉场扩散作用下HPT极化的结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Effect of Anomalous Cross-Field Diffusion on the Field-Aligned Current Generation
First, on the basis of the satellite observations of the broadband electrostatic noise and the Alfven wave noise in the auroral magnetosphere, within a frame of the quasi-linear theory we show that the proton (anomalous cross-field) diffusion coefficient averaged over the flux tube is likely to reach a significant fraction of the Bohm rate at least in the disturbed periods. Second, as an extension of recently proposed model that a pair of the region 1 and region 2 field-aligned currents (FACs) can be generated as a result of "natural distortion" of the hot plasma torus (HPT) in the magnetosphere under the influence of the usually prevailing convection with twin vortex cells (when the interplanetary magnetic field (IMF) is southward), we study the possible effect of the anomalous cross-field diffusion on the large-scale FACs resulting from the HPT polarization. In the magnetosphere, the hot (≥ 1 keV) plasma particles are primarily distributed in a magnetic shell which is connected to two ovals of diffuse auroras on the northern and southern polar ionospheres. Such hot plasma population is called the hot plasma torus (HPT). The numerical calculations specifically show that primary modification of the FAC pattern by this effect is the appearance of the triple FAC structure (i.e., upward FAC zone sandwiched between two downward FAC zones) in the midnight sector, which can be identified from the satellite observations at least during substorm periods. As a direct consequence of formation of such a triple FAC structure, the Harang discontinuity appears in the electric potential pattern. Thus the formation of the Harang discontinuity can be understood as a result of the HPT polarization by both effects of magnetic drift and anomalous cross-field diffusion.
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