正则化kappa分布的平行电磁模线性色散理论

E. Husidic, M. Lazar, H. Fichtner, K. Scherer, P. Astfalk
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引用次数: 13

摘要

在空间等离子体中原位测量的速度粒子分布偏离了麦克斯韦(热平衡),表现出标准kappa分布(SKD)所描述的增强的超热尾。尽管SKD的应用取得了成功,但由于一系列非物理含义,如速度矩的发散,阻碍了对等离子体的宏观描述,因此经常引起争议。正则化kappa分布(RKD)的引入克服了这些限制,但RKD等离子体的色散特性尚未得到研究。在本文中,我们计算了以RKD为特征的等离子体中电磁模式的频率频散和衰减或增长速率的波数。这项任务是通过使用基于网格的动力学色散求解器LEOPARD来完成的,该求解器是为任意陀螺向分布而开发的[P]。Astfalk和F. Jenko, J.地球物理学。Res. 122, 89(2017)]。通过再现先前为SKD和maxwell获得的结果,我们验证了代码的功能。此外,我们应用各向同性和各向异性RKDs来研究稳定的电磁电子回旋加速器(EMEC)和离子回旋加速器(EMIC)模式以及温度各向异性驱动的不稳定性,包括$T_\perp / T_\parallel > 1$ (EMEC和EMIC不稳定性)和$T_\perp / T_\parallel < 1$(质子和电子火龙带不稳定性)。其中$\parallel$和$\perp$表示与本地时均磁场平行和垂直的方向。如果截断参数$\alpha$足够小,结果表明RKDs在定性和定量水平上都能再现SKD等离子体的色散曲线。然而,对于较高的值,会发生物理上显著的偏差。
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Linear dispersion theory of parallel electromagnetic modes for regularized Kappa-distributions
The velocity particle distributions measured in-situ in space plasmas deviate from Maxwellian (thermal) equilibrium, showing enhanced suprathermal tails which are well described by the standard Kappa-distribution (SKD). Despite its successful application, the SKD is frequently disputed due to a series of unphysical implications like diverging velocity moments, preventing a macroscopic description of the plasma. The regularized Kappa-distribution (RKD) has been introduced to overcome these limitations, but the dispersion properties of RKD-plasmas are not explored yet. In the present paper we compute the wavenumber dispersion of the frequency and damping or growth rates for the electromagnetic modes in plasmas characterized by the RKD. This task is accomplished by using the grid-based kinetic dispersion solver LEOPARD developed for arbitrary gyrotropic distributions [P. Astfalk and F. Jenko, J. Geophys. Res. 122, 89 (2017)]. By reproducing previous results obtained for the SKD and Maxwellian, we validate the functionality of the code. Furthermore, we apply the isotropic as well as the anisotropic RKDs to investigate stable electromagnetic electron-cyclotron (EMEC) and ion-cyclotron (EMIC) modes as well as temperature-anisotropy-driven instabilities, both for the case $T_\perp / T_\parallel > 1$ (EMEC and EMIC instabilities) and for the case $T_\perp / T_\parallel < 1$ (proton and electron firehose instabilities), where $\parallel$ and $\perp$ denote directions parallel and perpendicular to the local time-averaged magnetic field. Provided that the cutoff parameter $\alpha$ is small enough, the results show that the RKDs reproduce the dispersion curves of the SKD plasmas at both qualitative and quantitative levels. For higher values, however, physically significant deviation occurs.
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