首页> 外文期刊>Journal of Geophysical Research, A. Space Physics: JGR >Ground-based magnetometer determination of in situ Pc4-5 ULF electric field wave spectra as a function of solar wind speed
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Ground-based magnetometer determination of in situ Pc4-5 ULF electric field wave spectra as a function of solar wind speed

机译:地面磁力仪测定原位Pc4-5 ULF电场波光谱作为一个太阳风速度的函数

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We present a statistical characterization of ground-based ultra-low-frequency mHz) magnetic wave power spectral densities (PSDs) as a function of latitude (corresponding to dipole L-shells from L.-2.5-8), local time, and solar wind speed. We show a clear latitudinal dependence on the PSD profiles, with PSDs increasing monotonically from low- to auroral zone latitudes, where PSDs are peaked before decay in amplitude at higher latitudes. In general, ULF wave powers are highest on the nightside, followed by the local morning, noon, and finally dusk sectors, and are well-characterized and well-ordered by solar wind speed at all MLTs spanning L~2.5-8. A distinct peak in PSD in the 2-8 mHz frequency range above a background power law is evident at most stations studied in this paper, demonstrating a significant non power law like component in the ULF wave power spectrum, in particular at high solar wind speeds. We conclude that field line resonance (FLR) behavior in the magnetosphere is most likely responsible for the peak in PSD, and that such peaks should be included in any radiation belt radial diffusion model addressing radiation belt dynamics. Furthermore, we utilize a model in order to map the ground-based magnetic ULF wave power measurements into electric fields in the equatorial plane of an assumed dipole magnetic field, and find excellent agreement with the in situ CRRES electric fields shown by Brautigam et al. [2005], clearly demonstrating the utility of ground-based measurements in providing reliable estimates of ULF electric field PSD for nowcast input into radiation belt radial diffusion models.
机译:我们的统计特性地面ultra-low-frequency mHz)磁波功率谱密度(psd)纬度的函数(对应于偶极子L-shells l - 2.5 - 8),当地时间和太阳能风速。依赖PSD文件,PSDs会从低收入到极光单调增加区纬度,PSDs前达到顶峰衰变振幅在高纬度地区。一般情况下,ULF波上最高权力阴面,紧随其后的是当地的早晨,中午,最后黄昏行业,特征明显,秩序井然的太阳风所有传输速度生成L ~ 2.5 8。峰在PSD上面的2 - 8 mHz频率范围背景幂律是显而易见的站研究,展示显著的非幂律的组件ULF波功率谱,尤其是在高太阳风速度。磁气圈是共振(FLR)行为最有可能负责PSD的,应该包含在任何这样的山峰辐射带径向扩散模型解决辐射带动态。为了映射模型地面磁ULF波功率测量电场赤道平面的一个假定的偶极子磁场,并找到优秀的协议所示的原位crr电场布劳提根等。[2005],清楚地展示地面测量的实用程序提供可靠的估计ULF电气场PSD的短时预测输入需要美国所有企业提供辐射带径向扩散模型。

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