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首页> 外文期刊>Icarus: International Journal of Solar System Studies >Ground-based observations of Saturn's auroral ionosphere over three days: Trends in HI temperature, density and emission with Saturn local time and planetary period oscillation
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Ground-based observations of Saturn's auroral ionosphere over three days: Trends in HI temperature, density and emission with Saturn local time and planetary period oscillation

机译:三天内对土星极光电离层的地面观测:土星局部时间和行星周期振荡引起的高温,密度和发射趋势

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摘要

On 19-21 April 2013, the ground-based 10-m W.M. Keck II telescope was used to simultaneously measure HI emissions from four regions of Saturn's auroral ionosphere: (1) the northern noon region of the main auroral oval; (2) the northern midnight main oval; (3) the northern polar cap and (4) the southern noon main oval. The H-3(+) emission from these regions was captured in the form of high resolution spectral images as the planet rotated. The results herein contain twenty-three H-3(+) temperatures, column densities and total emissions located in the aforementioned regions - ninety-two data points in total, spread over timescales of both hours and days. Thermospheric temperatures in the spring-time northern main oval are found to be cooler than their autumn-time southern counterparts by tens of K, consistent with the hypothesis that the total thermospheric heating rate is inversely proportional to magnetic field strength. The main oval H-3(+) density and emission is lower at northern midnight than it is at noon, in agreement with a nearby peak in the electron influx in the post-dawn sector and a minimum flux at midnight. Finally, when arranging the northern main oval H-3(+) parameters as a function of the oscillation period seen in Saturn's magnetic field the planetary period oscillation (PPO) phase - we see a large peak in H-3(+) density and emission at similar to 115 degrees northern phase, with a full-width at half-maximum (FWHM) of similar to 44 degrees. This seems to indicate that the influx of electrons associated with the PPO phase at 90 is responsible at least in part for the behavior of all H(3)(+)parameters. A combination of the H-3(+) production and loss timescales and the 10 uncertainty in the location of a given PPO phase are likely, at least in part, to be responsible for the observed peaks in H-3(+) density and emission occurring at a later time than the peak precipitation expected at 90 PPO phase. (C) 2015 Elsevier Inc. All rights reserved.
机译:2013年4月19日至21日,地面基准点为Keck II望远镜用于同时测量土星极光电离层四个区域的HI发射:(1)主要极光椭圆的北正午区域; (2)午夜北部主要椭圆形; (3)北极帽和(4)南部正午主椭圆形。随着行星旋转,以高分辨率光谱图像的形式捕获了来自这些区域的H-3(+)发射。本文的结果包含位于上述区域的23个H-3(+)温度,色谱柱密度和总排放量-总共92个数据点,分布在小时和天的时间范围内。发现春季北部主要椭圆形的热层温度比秋季南部南部的椭圆形低几十个K,这与热球总加热速率与磁场强度成反比的假设相一致。椭圆形的主要H-3(+)密度和发射在午夜北部比中午要低,这与黎明后区域电子流入附近的峰值和午夜的最小通量相符。最后,当将北部主要椭圆形H-3(+)参数设置为土星磁场中振荡周期,行星周期振荡(PPO)相的函数时,我们会看到H-3(+)密度出现一个大峰值,发射类似于北纬115度,半峰全宽(FWHM)约为44度。这似乎表明与PPO相在90°相伴的电子涌入至少部分负责所有H(3)(+)参数的行为。 H-3(+)产生和损失时标以及给定PPO相位置的10个不确定性的组合可能至少部分地导致了H-3(+)密度和排放发生在比90 PPO阶段预期的峰值降水晚的时间。 (C)2015 Elsevier Inc.保留所有权利。

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