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Dispersion relation for electron waves propagating in an isotropic plasma containing Maxwellian and suprathermal electrons

机译:在包含麦克斯韦和超热电子的各向同性等离子体中传播的电子波的色散关系

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摘要

The paper discusses the dispersion relation for longitudinal electron waves propagating in a collisionless, homogeneous isotropic plasma, which contains both Maxwellian and suprathermal electrons. I t is found that the dispersion curve, known to have two separate branches for zero suprathermal energy spread,depends sensitively on this quantity. As the energy half-width of the suprathermaludpopulation increases, the branches approach each other until they touch at a connexion point, for a small critical value of that half-width. The topology of the dispersion curves is different for half-widths above and below critical; and this can affect the use of wave-propagation measurements as a diagnostic technique for the determination of the electron distribution function. Both the distance between the branches and spatial damping near the connexion frequency depend on the half-width, if below critical, and can be used to determine it. The theory is applied to experimental data.
机译:本文讨论了在无碰撞的均质各向同性等离子体中传播的纵向电子波的色散关系,该等离子体同时包含麦克斯韦电子和超热电子。我们发现,色散曲线(已知有两个独立的分支,用于零超热能扩散)敏感地取决于该量。随着超热人口的能量半峰宽度的增加,分支彼此接近,直到它们在连接点接触为止,以获得该半峰宽度的较小临界值。对于高于和低于临界值的半角宽度,色散曲线的拓扑是不同的。这会影响将波传播测量作为确定电子分布函数的诊断技术的使用。分支之间的距离和连接频率附近的空间阻尼都取决于半宽度(如果低于临界值),可以用来确定半宽度。该理论适用于实验数据。

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