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Geomagnetic activity and local time dependence of the distribution of ultra low-frequency wave power in azimuthal wavenumbers, m

机译:地波数m中超低频波功率分布的地磁活动和当地时间依赖性

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摘要

The azimuthal wavenumber of ultra low-frequency (ULF) waves in themagnetosphere is a required parameter in the calculations of the diffusionrates of energetic electrons and protons in the magnetosphere, as electronsand protons of drift frequency have been shown to radiallydiffuse due to resonant interaction with ULF waves of frequency  = . However, there are difficulties in estimating , due tolack of multipoint measurements. In this paper we use magnetic fieldmeasurements at geosynchronous orbit to calculate the cross-spectrogram powerand phase differences between time series from magnetometer pairs.Subsequently, assuming that ULF waves of a certain frequency and would beobserved with a certain phase difference between two azimuthally alignedmagnetometers, the fraction of the total power in each phase difference rangeis calculated. As part of the analysis, both quiet-time and storm-timedistributions of power per number are calculated, and it is shown thatduring active times, a smaller fraction of total power is confined to lower than during quiet times. It is also shown that in the dayside region,power is distributed mostly to the lowest azimuthal wavenumbers  = 1 and2, whereas on the nightside it is more equally distributed to all thatcan be resolved by the azimuthal separation between two spacecraft.
机译:磁流层中超低频(ULF)波的方位角波数是计算磁层中高能电子和质子扩散率的必要参数,因为已证明漂移频率的电子和质子由于与ULF的共振相互作用而径向扩散频率为=的波。但是,由于缺乏多点测量,因此难以估算。在本文中,我们使用地球同步轨道上的磁场测量来从磁力计对计算时间序列之间的互谱图功率和相位差。计算每个相位差范围内的总功率的分数。作为分析的一部分,计算了每个功率的静默时间和风暴时间分布,结果表明,在活动时间内,总功率的一小部分被限制为低于静默时间。还表明,在白天区域,功率主要分配给最低的方位波数= 1和2,而在夜间,功率分配更均等地分配给两个航天器之间可以通过方位分离解决的所有问题。

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