赤道等离子体气泡的纬向分布:高度变异

L. Sidorova
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摘要

本文研究了赤道等离子体气泡的纬向分布及其随观测高度的变化规律。为此,对不同海拔高度获得的EPB发生概率的纬度直方图进行了详细的对比分析。来自ISS-b(~ 972−1220公里)、ROCSAT-1(~ 600公里)和AE-E(~ 350−475公里)航天器的数据被用于此目的。从ISS-b数据中确定EPB结构为He密度耗尽,从ROCSAT-1和AE-E数据中确定EPB结构为离子密度(Ni)耗尽。在高太阳活动年份的不同季节条件下进行了考虑。结果表明,随着观测高度从~ 600km增加到~ 1000km, EPB发生概率直方图除赤道极大值外,还出现了中纬度极大值。这一特征在秋分时期的半球和冬季半球都最为明显。在上层电离层高度(~ 972 ~ 1220km, ISS-b), EPB发生概率的中纬度最大值与赤道最大值相当或开始占主导地位。这一特征在所有季节的观测中都是典型的。结果表明,随着观测高度的增加,中纬度极暴发生概率最大值的纬度位置向赤道偏移。后者很好地符合磁场管的纬度路线,等离子体气泡沿着磁场管伸展,这些磁场管已经达到了它们的天花板高度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Latitudinal distribution of the equatorial plasma bubbles: Altitude variability
In this paper, the latitudinal distributions of the equatorial plasma bubbles (EPBs) and their variability with the observation heights were studied. For this purpose, a detailed comparative analysis of the latitudinal histograms of the EPB occurrence probability obtained at the different altitudes was performed. The data from the ISS-b (∼ 972− 1220km) ROCSAT-1 (∼ 600km) and AE-E (∼ 350− 475km) spacecrafts were used for this purpose. The EPB structures were identified from the ISS-b data as the He density depletions, and from the ROCSAT-1 and AE-E data as the ion density (Ni) depletions. Different seasons during the years of the high solar activity conditions were under consideration. It was obtained that as the observation height increases from ∼ 600km to ∼ 1000km, the mid-latitude maxima in addition to the equatorial maximum develop in the histograms of the EPB occurrence probability. This feature was most pronounced in both the hemispheres of the equinox periods and in the winter hemispheres. At the altitudes of the upper topside ionosphere (∼ 972 − 1220km, ISS-b), the values of the mid-latitude maxima of the EPB occurrence probability become comparable or begin to dominate in relation to the equatorial maximum. This feature is typical for all seasons of the observations. Moreover, it was obtained that the latitudinal positions of the mid-latitude maxima of the EPB occurrence probability shift to the equator with increase in the observation heights. The latter is in good accordance with the latitudinal courses of the magnetic field tubes along which the plasma bubbles that have already reached their ceiling heights are stretched.
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