日本地球惑星科学連合2024年大会

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セッション記号 P (宇宙惑星科学) » P-EM 太陽地球系科学・宇宙電磁気学・宇宙環境

[P-EM12] Coupling Processes in the Atmosphere-Ionosphere System

2024年5月30日(木) 09:00 〜 10:15 展示場特設会場 (2) (幕張メッセ国際展示場 6ホール)

コンビーナ:細川 敬祐(電気通信大学大学院情報理工学研究科)、Liu Huixin(九州大学理学研究院地球惑星科学専攻 九州大学宙空環境研究センター)、大塚 雄一(名古屋大学宇宙地球環境研究所)、Chang Loren(Institute of Space Science, National Central University)、Chairperson:Thomas J Immel(University of California Berkeley)、大塚 雄一(名古屋大学宇宙地球環境研究所)

09:30 〜 09:45

[PEM12-03] Electron density depletion and electric field variation of plasma bubble observed by the Arase satellite during a geomagnetic storm in April 2023

*惣宇利 卓弥1新堀 淳樹1堀 智昭1大塚 雄一1西岡 未知2Perwitasari Septi2笠羽 康正4熊本 篤志3土屋 史紀4松田 昇也5笠原 禎也5松岡 彩子6寺本 万里子7三好 由純1篠原 育8 (1.名古屋大学 宇宙地球環境研究所、2.情報通信研究機構、3.東北大学 理学研究科、4.東北大学 附属惑星プラズマ・大気研究センター、5.金沢大学、6.京都大学 地磁気センター、7.九州工業大学、8.宇宙航空研究開発機構 宇宙科学研究所)

キーワード:磁気嵐、全球測位衛星システム、あらせ衛星、プラズマバブル、電場

After sunset, a plasma density depletion (plasma bubble) often occurs at the bottom of the F region ionosphere over the dip equator. Plasma bubbles are sometimes extended from the equator to mid-latitudes during geomagnetic storms. An eastward electric field is one of the most important factors for generating plasma bubbles through the Rayleigh-Taylor instability. Plasma bubbles also move upward due to an eastward polarization electric field generated inside them with the northward geomagnetic field. The large-sale evolution of plasma bubbles was extensively studied using ground and satellite observations, whereas there have been few direct observations of the electric field inside plasma bubbles during geomagnetic storms. In this study, we clarify a possible generation mechanism of equatorial plasma bubbles extending to the mid-latitudes during a geomagnetic storm in April 2023 by analyzing global navigation satellite system-total electron content (TEC), rate of TEC index (ROTI) and Arase satellite data.
During the main phase of the geomagnetic storm, equatorial plasma bubbles were generated in the European sector and extended to mid-latitudes of ~40° N in geomagnetic latitude. The plasma bubbles indicated by the ROTI enhancement extended northward and they tilted westward. The Arase satellite passed through the plasma bubbles and observed electron density depletions in the dusk sector (20–21.5 h MLT) around 15° N in geomagnetic latitude at an altitude of 450–700 km. Some of the density depletions correspond to the enhanced ROTI regions related to the plasma bubbles. One of the electron density variations showed a sharp depletion from 9.84×1011 m-3 to 1.68×109 m-3. An electric field enhancement was also observed by the Arase satellite when it passed through one of the density depletion regions. This is the first time that Arase has identified the eastward electric field enhancement inside storm-time plasma bubbles. The observed electric field shows a perturbation in the northward, upward, and eastward directions in solar magnetic coordinates. The amplitude of the eastward (polarization) electric field was ~25 mV/m, which corresponds to the upward velocity of ~480 m/s. On the other hand, some previous studies have reported observations of the upward velocity (eastward electric field) related to plasma bubbles using satellite or radar data and shown that the amplitude of the E×B velocity was a few hundred m/s. This suggests that the upward velocity inside the plasma bubbles was more intensified during the geomagnetic storm as compared with that during geomagnetically quiet times. This is because the penetration electric field in the equatorial region is further enhanced during geomagnetic storms. In the equatorial region, the charge separation in the electron density perturbation region can be enhanced by the enhanced eastward Pedersen current driven by the eastward electric field, generating a larger polarization electric field to hold the current continuity. Our analysis results would contribute to the understanding of the development mechanism of plasma bubbles extending to the mid-latitudes during geomagnetic storms.