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Kinetic Alfven wave driven by the density inhomogeneity in the presence of loss-cone distribution function—particle aspect analysis

机译:损失锥分布函数存在下由密度不均匀性驱动的动力学阿尔夫文波—颗粒长宽比分析

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摘要

Kinetic Alfven waves (KAWs) driven by the diamagnetic drift instability that is excited by the density inhomogeneity in low-β plasmas, such as plasmas in the auroral region, are investigated by adopting the particle aspect analysis and loss-cone distribution function. The results obtained in this paper indicate that the propagation and evolution of kinetic Alfven waves decrease and the kinetic Alfven wave excitation becomes not easier with increasing loss-cone index J. But the spatial scales of the perpendicular perturbation driving kinetic Alfven waves have a decreasing tendency with the larger values of J, which perhaps is in relation with the decreasing width of loss-cone. A single hump appears in the plots of the growth rate of the instability when J = 2. But the hump cannot emerge when J = 0 or J = 1. The density inhomogeneity of ions plays an important role in driving KAWs and it cannot be ignored. KAWs can be easier driven and KAWs can propagate and evolve faster with the increasing level of density inhomogencity. However, the range of the perpendicular wave number of the wave instability decreases, namely, the longer the scale of perpendicular disturbance the easier the excitation of KAW. As the density inhomogeneity increases, the tendency of numerical solutions of the dispersion relation is similar to that obtained by the kinetic theory and Maxwellian distribution function (Duan and Li, 2004). But the profiles of the plots of numerical solutions are different. This means that the velocity distribution function of particles is important for KAW driven in magnetoplasmas, especially in the active regions of the magnetosphere, such as auroral region, and plasma sheet boundary.
机译:通过采用粒子长宽比分析和损失锥分布函数,研究了由低β等离子体(如极光区域中的等离子体)的密度不均匀性激发的反磁漂移不稳定性驱动的动力学Alfven波(KAW)。本文获得的结果表明,随着损耗锥指数J的增加,动力学Alfven波的传播和演化减小,并且动力学Alfven波的激发变得不容易。但是,垂直扰动驱动动力学Alfven波的空间尺度具有减小的趋势J的值较大,这可能与损耗锥的宽度减小有关。当J = 2时,不稳定性的增长率图中会出现一个驼峰。但是当J = 0或J = 1时,驼峰就不会出现。离子的密度不均匀性在驱动KAW中起着重要作用,因此不容忽视。 。随着密度不均匀性水平的提高,KAW可以更容易驱动,并且KAW可以更快地传播和进化。但是,波不稳定性的垂直波数的范围减小,即,垂直扰动的范围越长,KAW的激发越容易。随着密度不均匀性的增加,色散关系数值解的趋势与动力学理论和麦克斯韦分布函数得到的结果相似(Duan和Li,2004)。但是数值解的图的轮廓是不同的。这意味着粒子的速度分布函数对于在磁浆中驱动的KAW非常重要,尤其是在磁层的活动区域(如极光区域和等离子片边界)中。

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