亚极光纬度的孤立质子极光和Pc1/EMIC波

K. Sakaguchi, K. Shiokawa, Y. Miyoshi, M. Connors
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引用次数: 14

摘要

亚极光电离层中的孤立质子极光(IPA)是由高能质子通过波粒相互作用与共轭内磁层中的电磁离子回旋波(EMIC)产生的。本研究利用2006-2012年加拿大阿萨巴斯卡地区的地面成像数据,统计研究了ipa的空间分布和发生概率,并以此作为主震波发生区域的代表。在整个观测区间内,IPA发生概率的7年平均值为0.83%,最大年与最小年之间的变化因子为5。当地时间(16至06时)分布在午夜前和黄昏出现双峰。发生概率随Kp的增加而增加,MLT的位置有向暗方向移动的趋势。IPA大小的统计分布在1万km 2的空间大小处有一个明显的峰值,在电离层高度处,纬度和纵向长度分别在56 km和340 km处有一个峰值。利用磁场示踪估计了IPA震源位置和二维结构的赤道投影。这些空间结构对于定量估计高能粒子的损失率至关重要,有助于空间天气研究。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Isolated Proton Auroras and Pc1/EMIC Waves at Subauroral Latitudes
Isolated proton aurora (IPA) in the subauroral ionosphere is created by energetic proton precipitation through wave-particle interactions with electromagnetic ion cyclotron (EMIC) waves in the conjugate inner magnetosphere. In this study, spatial distribution and occurrence probability of IPAs were statistically investigated as a proxy for regions of EMIC wave occurrence using ground-based imaging data in 2006-2012 at Athabasca, Canada. The seven-year average of the IPA occurrence probability over the total observation interval was estimated to be 0.83% and a factor of five change was found between maximum and minimum years. Local time (between 16 and 06 MLT) distribution shows double peaks at pre-midnight and at dusk. The occurrence probability increases with Kp and the MLT location tends to shift duskward. The statistical distribution of IPA size shows a clear peak at a spatial size of 10,000 km 2 , and latitudinal and longitudinal lengths have peaks at 56 and 340 km, respectively, at the ionospheric altitude. The equatorial projections of IPA source locations and two-dimensional structures are estimated by mag-netic field tracing. These spatial structures are essential to quantitatively estimate the loss rate of energetic particles, contributing to space weather studies.
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