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Sensitive Dependence of Ultrarelativistic Electron Precipitation on EMIC Wave Frequency

机译:敏感的依赖Ultrarelativistic电子降水在位的波的频率

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Electromagnetic ion cyclotron (EMIC) waves have long been considered to cause atmospheric precipitation loss of relativistic electrons, the quantitative evaluation of which is critical for understanding the radiation belt electron flux dropouts. In this study, we report test particle calculation results on precipitation loss rates of 5 MeV electrons with initial pitch angles of 4–10° at the equator by He+ band EMIC waves. We find a sensitive dependence of the precipitation loss rates on the wave frequency in that a preferred wave frequency (maximum loss frequency) exists at which the loss rate peaks predominantly and away from which it declines substantially. According to a cold plasma dispersion relation, a small difference in wave frequency just below the He+ gyrofrequency corresponds to a significant difference in wavenumber. Different frequencies lead to phase trapping of different extents, which determines the significance of loss cone scattering at the exit latitude from the wave zone. At frequencies below the maximum loss frequency, phase trapping causes large advective pitch angle changes, prohibiting loss cone scattering. At the maximum loss frequency, the phase-trapping effect is optimized such that diffusion is dominant over advection and large enough to allow effective loss cone scattering. At frequencies above the maximum loss frequency, the phase-trapping effect disappears, and the resulting (both diffusive and advective) scattering is too weak to drive loss cone scattering unless the initial pitch angle is close enough to the loss cone angle.
机译:电磁离子回旋波位的长期以来被认为是导致大气相对论电子的沉淀损失定量评价的关键了解辐射带电子通量辍学。在降水损失率计算结果5兆电子伏电子初始螺距角由他+ 4到10°在赤道带位的波。找到一个敏感的依赖降水亏损率在一个波的频率喜欢波频率(最大损失频率)存在的损失率山峰为主,远离它大幅下降。根据冷等离子体色散关系,在波频率略低于小差别他+旋转频率对应于一个重要不同波数。导致相位捕获不同的区段,决定损失锥的意义吗在出口处散射波的纬度区。频率、相位捕获大型平流引起螺旋角变化,禁止损失锥散射。phase-trapping效应等进行了优化扩散是在平流和大占主导地位足以让有效的散射损失锥。以上频率的最大损失频率,phase-trapping效应消失,结果(包括扩散和对流)太弱散射损失锥散射,除非最初的螺旋角足够接近损失锥角。

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