Che H, Schiff C, Le G, Dorelli J, Giles B, Moore T
University of Maryland, College Park, MD, 20742, USA.
NASA Goddard Space Flight Center, Greenbelt, MD, 20771, USA.
Phys Plasmas. 2018 Mar;25(3). doi: 10.1063/1.5016853. Epub 2018 Mar 1.
In space plasma, various effects of magnetic reconnection and turbulence cause the electron motion to significantly deviate from their Larmor orbits. Collectively these orbits affect the electron velocity distribution function and lead to the appearance of the "non-gyrotropic" elements in the pressure tensor. Quantification of this effect has important applications in space and laboratory plasma, one of which is tracing the electron diffusion region (EDR) of magnetic reconnection in space observations. Three different measures of agyrotropy of pressure tensor have previously been proposed, namely, ∅ , and . The multitude of contradictory measures has caused confusion within the community. We revisit the problem by considering the basic properties an agyrotropy measure should have. We show that ∅ , and are all defined based on the sum of the principle minors (i.e. the rotation invariant ) of the pressure tensor. We discuss in detail the problems of -based measures and explain why they may produce ambiguous and biased results. We introduce a new measure constructed based on the determinant of the pressure tensor (i.e. the rotation invariant ) which does not suffer from the problems of -based measures. We compare with other measures in 2 and 3-dimension particle-in-cell magnetic reconnection simulations, and show that can effectively trace the EDR of reconnection in both Harris and force-free current sheets. On the other hand, ∅ does not show prominent peaks in the EDR and part of the separatrix in the force-free reconnection simulations, demonstrating that ∅ does not measure all the non-gyrotropic effects in this case, and is not suitable for studying magnetic reconnection in more general situations other than Harris sheet reconnection.
在空间等离子体中,磁重联和湍流的各种效应导致电子运动显著偏离其拉莫尔轨道。这些轨道共同影响电子速度分布函数,并导致压力张量中出现“非旋转变换”元素。这种效应的量化在空间和实验室等离子体中具有重要应用,其中之一是在空间观测中追踪磁重联的电子扩散区域(EDR)。此前已经提出了三种不同的压力张量非旋转变换度量,即∅ 、 和 。众多相互矛盾的度量在该领域内造成了混乱。我们通过考虑非旋转变换度量应具备的基本属性来重新审视这个问题。我们表明,∅ 、 和 都是基于压力张量的主子式之和(即旋转不变量 )来定义的。我们详细讨论了基于 的度量存在的问题,并解释了它们为何可能产生模糊和有偏差的结果。我们引入了一种基于压力张量行列式(即旋转不变量 )构建的新度量 ,它不存在基于 的度量所存在的问题。我们在二维和三维粒子模拟磁重联中,将 与其他度量进行了比较,结果表明 能够有效地追踪哈里斯电流片和无力电流片中重联的EDR。另一方面,在无力重联模拟中,∅ 在EDR和部分分隔线上并未显示出明显的峰值,这表明在这种情况下,∅ 并未测量到所有的非旋转变换效应,并且不适用于研究除哈里斯电流片重联之外的更一般情况下的磁重联。