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Variation of the Martian Ionospheric Electron Density from Mars Express Radar Soundings

机译:火星快车雷达探测到的火星电离层电子密度的变化

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摘要

The Mars Advanced Radar for Subsurface and Ionospheric Sounding aboard Mars Express has been in operation for over 2 years. Between 14 August 2005 and 31 July 2007, we obtain 34,492 ionospheric traces, of which 14,060 yield electron density profiles and 12,291 yield acceptable fits to the Chapman ionospheric model. These results are used to study the Martian ionosphere under changing conditions: the presence or absence of solar energetic particles, solar EUV flux, season, solar zenith angle, and latitude. The 2-year average subsolar maximum electron density n 0 is 1.62 × 105 cm−3, the average subsolar electron density altitude h 0 is 128.2 km, and the average neutral scale height H is 12.9 km. Solar energetic particle events are associated with a 6% increase in n 0, a 3 km decrease in h 0, and a 0–7 km decrease in H. The value of n 0 varies smoothly between 1.4 × 105 and 1.8 × 105 cm−3, yielding d ln n 0/d ln F10.7 = 0.30 ± 0.4; h 0 varies between 115 and 135 km, while H remains relatively constant with EUV flux and season, in contrast with previous work. The value of h 0 decreases toward the terminator at low latitude but increases poleward during summer; H varies from 11 km, for solar zenith angle less than 40°, to between 14 and 17 km near the terminator, depending on season. Near-peak temperatures vary between 220 K and 300 K, less variation than indicated by modeling, probably due to sampling near solar minimum.
机译:火星快车上用于地下和电离层探测的火星高级雷达已经运行了两年以上。在2005年8月14日至2007年7月31日期间,我们获得了34,492个电离层迹线,其中有14,060个产生的电子密度分布图和12,291个合格的对Chapman电离层模型的拟合。这些结果用于研究变化条件下的火星电离层:是否存在太阳高能粒子,太阳EUV通量,季节,太阳天顶角和纬度。两年的平均日太阳最大电子密度n 0为1.62×105 cm-3,平均日太阳电子密度高度h 0为128.2 km,平均中性尺度高度H为12.9 km。太阳高能粒子事件与n 0增大6%,h 0减小3 km和H减小0-7 km有关。n0的值在1.4×105和1.8×105 cm−之间平稳变化3,屈服d ln n 0 / d ln F10.7 = 0.30±0.4; h 0在115至135 km之间变化,而H与EUV通量和季节保持相对恒定,这与以前的工作相反。 h 0的值在低纬度时朝向终止子减小,但在夏季极向增大; H值从11 km(太阳天顶角小于40°)变化到终止器附近的14至17 km之间(视季节而定)。近峰温度在220 K至300 K之间变化,变化幅度小于模型指示的变化,这可能是由于接近太阳极小值的采样所致。

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