论文标题

将磁重新连接生长的阶段与无碰撞等离子体中X线结构的时间演化有关

Relating the Phases of Magnetic Reconnection Growth to the Temporal Evolution of X-line Structures in a Collisionless Plasma

论文作者

Payne, D. S., Torbert, R. B., Germaschewski, K., Forbes, T. G., Shuster, J. R.

论文摘要

磁重新连接期间能量转化的效率与重新连接率有关。虽然已经对稳定的重新连接率进行了广泛的研究,但在重新连接开始和峰重新连接率之间的增长尚未得到彻底讨论。我们使用2D粒子中的模拟(PIC)模拟来检查在生长过程中非理想重新连接的电场如何演变,以及它与X线附近的变化之间的关系。我们确定生长的三个阶段:1)慢速准线性生长,2)快速指数生长,3)重新连接率峰值后的锥形生长,然后是负增长。通过分析EDR的结构变化,我们将早期阶段与X线对称性相关联,通过侵蚀到X线对称性,通过侵蚀前双极性EZ以及在第1阶段中性线上的差异EX模式的出现,然后在流入区域的扩展和EIN的迅速增长中,越来越多地与空间相关。在第2阶段,通过打开排气,缓解电子规模的瓶颈,并允许在分离板上进行大量的po液通量。我们发现电磁能的快速流入累积,直到第3阶段的下游电磁能密度接近初始上游渐近值。最后,我们研究了电子流出和下游离子种群如何在第3阶段相互作用,以及每个物种如何与排气中的局部场结构交换能量。

The efficiency of energy conversion during magnetic reconnection is related to the reconnection rate. While the stable reconnection rate has been studied extensively, its growth between the time of reconnection onset and the peak reconnection rate has not been thoroughly discussed. We use a 2D particle-in-cell (PIC) simulation to examine how the non-ideal reconnection electric field evolves during the growth process and how it relates to changes near the x-line. We identify three phases of growth: 1) slow quasi-linear growth, 2) rapid exponential growth, and 3) tapered growth followed by negative growth after the reconnection rate peaks. Through analysis of the structural changes of the EDR, we associate the early phases with the breaking of x-line symmetry through the erosion of the pre-onset bipolar Ez and the emergence of a diverging Ex pattern at the neutral line in phase 1 followed by the expansion of the inflow region and the enhancement of inflow Poynting flux Sz associated with the out-of-plane electric field Ey in phase 2. We show how the Hall fields facilitate rapid growth in phase 2 by opening up the exhaust, relieving the electron-scale bottleneck and allowing large Poynting flux across the separatrices. We find that the rapid inflow of electromagnetic energy accumulates until the downstream electromagnetic energy density in phase 3 approaches the initial upstream asymptotic value. Finally, we examine how the electron outflow and the downstream ion populations interact in phase 3 and how each species exchanges energy with the local field structures in the exhaust.

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