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Fine scale structures of pulsating auroras in the early recovery phase of substorm using ground-based EMCCD camera

机译:小尺度结构的脉动极光亚暴使用的早期恢复阶段地面EMCCD相机

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[1]We have carried out ground-based observations, optimized to temporal and spatial characteristics of pulsating auroras (PAs) in the micro/meso scale, using an electron multiplying charge coupled device (EMCCD) camera with a wide field of view corresponding to 100 × 100 km at an altitude of 110 km and a high sampling rate up to 100 frames per second. We focus on transient PAs propagating southward around 1100 UT, in the early recovery phase of the substorm, on 4th March 2011. Three independent patches(PA1-3)each with different periods between 4 and 7 s were observed, which means that the periodicity was not explained by the electron bounce motion and strongly depended on local plasma conditions in the magnetosphere or in the ionosphere. One more insight is that only PA1 had also a sharp peak of modulations around 1.5 Hz, with a narrow frequency width of 0.30 Hz, and the strong modulations existed as a small spot in the center of PA1. We have also conducted cross spectrum analysis and have obtained coherence and phase distributions for auroral variations between 0.1 and 3.0 Hz. The results indicated that low frequency variations from 0.2 to 0.5 Hz inside PA1-3 propagated as a collective motion in well-defined directions. The estimated horizontal propagation velocities ranged from 50 to 120 km/s at the auroral altitude. The velocities are almost consistent with the Alfven speed at the magnetic equator, which suggests that compressional waves have an effect on PA via modulations of the ambient plasma environment.
机译:[1]我们已经进行了地面观测,优化的时间和空间特征脉动极光(PAs)的微/内消旋规模,使用一个电子倍增耦合装置(EMCCD)用广角镜头的对应于一个100×100公里110公里的高度和高采样率100帧每秒。向南传播约1100 UT,早期恢复阶段的亚暴,4日2011年3月。4和7 s之间的不同时期观察到,这意味着周期性不解释的电子运动和反弹强烈依赖于当地的等离子体条件磁气圈或电离层。洞察力是只有PA1也急剧的峰值调节约1.5赫兹,缩小0.30赫兹的频率宽度,强壮的人调节存在一个小点的中心PA1。分析和取得连贯性和阶段分布在极光0.1之间变化和3.0赫兹。从0.2到0.5 Hz频率变化PA1-3传播作为一个集体运动明确的方向。传播速度介于50到120 km / s在极光的高度。几乎与阿尔芬速度一致磁赤道,这表明压缩波在PA通过产生影响调节环境的等离子体环境。

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