Deriving the Ionospheric Electric Field From the Bulk Motion of Radar Aurora in the E-Region

IF 2.6 2区 地球科学 Q2 ASTRONOMY & ASTROPHYSICS
Magnus F. Ivarsen, Jean-Pierre St-Maurice, Devin R. Huyghebaert, Megan D. Gillies, Frank Lind, Brian Pitzel, Glenn C. Hussey
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Abstract

In the auroral E-region strong electric fields can create an environment characterized by fast plasma drifts. These fields lead to strong Hall currents which trigger small-scale plasma instabilities that evolve into turbulence. Radio waves transmitted by radars are scattered off of this turbulence, giving rise to the ‘radar aurora’. However, the Doppler shift from the scattered signal does not describe the F-region plasma flow, the E × B $\mathbf{E}\times \mathbf{B}$ drift imposed by the magnetosphere. Instead, the radar aurora Doppler shift is typically limited by nonlinear processes to not exceed the local ion-acoustic speed of the E-region. This being stated, recent advances in radar interferometry enable the tracking of the bulk motion of the radar aurora, which can be quite different and is typically larger than the motion inferred from the Doppler shift retrieved from turbulence scatter. We argue that the bulk motion inferred from the radar aurora tracks the motion of turbulent source regions (provided by auroras). This allows us to retrieve the electric field responsible for the motion of field tubes involved in auroral particle precipitation, since the precipitating electrons must E × B $\mathbf{E}\times \mathbf{B}$ drift. Through a number of case studies, as well as a statistical analysis, we demonstrate that, as a result, the radar aurora bulk motion is closely associated with the high-latitude convection electric field. We conclude that, while still in need of further refinement, the method of tracking structures in the radar aurora has the potential to provide reliable estimates of the ionospheric electric field that are consistent with nature.

Abstract Image

从 E 区域雷达极光的体运动推导电离层电场
在极光 E 区域,强电场会产生等离子体快速漂移的环境。这些电场会产生强大的霍尔电流,引发小尺度等离子体不稳定,进而演变成湍流。雷达发射的无线电波会从湍流中散射出来,形成 "雷达极光"。然而,散射信号的多普勒频移并不能描述 F 区等离子体流,即磁层施加的 E × B $\mathbf{E}\times \mathbf{B}$ 漂移。相反,雷达极光多普勒频移通常受到非线性过程的限制,不会超过 E 区的局部离子声速。尽管如此,雷达干涉测量法的最新进展使得跟踪雷达极光的整体运动成为可能,这种运动可能与从湍流散射中获取的多普勒频移推断的运动截然不同,而且通常更大。我们认为,从雷达极光推断出的体运动跟踪了湍流源区域的运动(由极光提供)。这使我们能够检索出极光粒子沉淀所涉及的场管运动的电场,因为沉淀电子必须 E × B $\mathbf{E}\times \mathbf{B}$ 漂移。通过大量的案例研究和统计分析,我们证明雷达极光的体运动与高纬度对流电场密切相关。我们的结论是,雷达极光结构跟踪方法虽然仍需进一步完善,但有可能提供与自然界一致的电离层电场可靠估计值。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Journal of Geophysical Research: Space Physics
Journal of Geophysical Research: Space Physics Earth and Planetary Sciences-Geophysics
CiteScore
5.30
自引率
35.70%
发文量
570
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