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首页> 外文期刊>Journal of Plasma Physics >Beam-plasma instability excited by non-thermal electrons with arbitrary distribution function and comparison with electron-cyclotron master
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Beam-plasma instability excited by non-thermal electrons with arbitrary distribution function and comparison with electron-cyclotron master

机译:具有任意分布函数的非热电子激发的束流等离子体不稳定性及其与电子回旋加速器的比较

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摘要

An equation is derived for the growth rates of. the beam-plasma instability excited by non-thermal electrons with arbitrary distribution function, and it is shown that the reactive instability does not depend on the assumption of a monoenergetie distribution. Hence the properties of electromagnetic waves are calculated for the hollow beam and loss-cone distribution functions. The general characteristics and structures of the growth rates are similar to the results for the rnonoenergetic distribution, but there are still some differences in the relation between the growth rates, and the relevant parameters, such us the ambient parameter (ol)e/?le, the angle of propagation 0 and the pitch angle a. The main purpose of this paper is to compare the properties of the beain-plasrna instability (reactive) and the electron-cyclotron inaser instability (kinetic) under similar ambient conditions. The calculations show that both kinds of instabilities are easily excited at larger angles of propagation with respect to the ambient magnetic field, which means that both depend mainly on the free energy of the non-thermal electrons perpendicular to the magnetic field. The Magnitudes of the growth rates of the two kinds of instabilities are comparable under the same ambient conditions. However, because the non-resonant wave—particle interaction is taken into consideration, for the beam-plasma instability, which makes the resonant peaks broaden and connect with each other, the spectra of the beam-plasma instability are also more complicated than that of the maser instability, and the range of the angle of propagation of the growing waves in the non-resonant case is also larger than that in the resonant case.
机译:推导了的增长率方程。由具有任意分布函数的非热电子激发的束-等离子体不稳定性,表明反应性不依赖于单能分布的假设。因此,计算了中空束和损耗锥分布函数的电磁波特性。增长率的一般特征和结构与微能量分布的结果相似,但是增长率与相关参数之间的关系仍然存在一些差异,例如环境参数(ol)e / le ,传播角为0,俯仰角为a。本文的主要目的是比较在相似环境条件下的贝恩等离子体不稳定性(反应性)和电子回旋加速器不稳定性(动力学)的性质。计算表明,相对于周围磁场,两种不稳定性都可以在较大的传播角度上轻易激发,这意味着两种不稳定性都主要取决于垂直于磁场的非热电子的自由能。在相同的环境条件下,两种不稳定性的增长率幅度是可比的。但是,由于考虑了非共振波与粒子的相互作用,因此,对于束状等离子体不稳定性,共振峰扩宽并相互连接,因此束状等离子体不稳定性的光谱也比束状等离子体不稳定性的光谱复杂。另外,在非共振情况下,由于脉动波的不稳定性,并且增长波的传播角度的范围也比共振情况下的大。

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