日本地球惑星科学連合2025年大会

講演情報

[E] ポスター発表

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

2025年5月25日(日) 17:15 〜 19:15 ポスター会場 (幕張メッセ国際展示場 7・8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)

17:15 〜 19:15

[PEM12-P18] Possible generation mechanism of plasma bubbles during a geomagnetic storm in April 2023 based on satellite observations and simulations

*惣宇利 卓弥1新堀 淳樹2堀 智昭2大塚 雄一2垰 千尋3陣 英克3横山 竜宏1西岡 未知3Perwitasari Septi3笠羽 康正5熊本 篤志4土屋 史紀5松田 昇也6笠原 禎也6松岡 彩子7寺本 万里子8山本 和弘2三好 由純2篠原 育9山本 衛1 (1.京都大学 生存圏研究所、2.名古屋大学 宇宙地球環境研究所、3.情報通信研究機構、4.東北大学 理学研究科、5.東北大学 附属惑星プラズマ・大気研究センター、6.金沢大学、7.京都大学 地磁気センター、8.九州工業大学、9.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、シミュレーション

Equatorial Plasma bubbles (EPBs) are sometimes expanded from the equator to mid-latitudes during geomagnetic storms. A background eastward electric field is one of the most important factors for generating EPBs through the Rayleigh-Taylor instability. The large-scale evolution of EPBs was extensively studied using ground and satellite observations. However, the development mechanism of storm-time EPBs to mid-latitudes is still unknown. In this study, we clarify a possible generation mechanism of EPBs expanding 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), Arase satellite data, Ground-to-topside model of Atmosphere and Ionosphere for Aeronomy (GAIA) model, and three-dimensional high-resolution bubble model.
The EPBs in the African-European longitudinal sector indicated by the ROTI enhancement expanded northward to mid-latitudes of ~40° N in geomagnetic latitude and they tilted westward with increasing latitude during the main phase of the geomagnetic storm. The Arase satellite passed through the EPBs and observed electron density depletions at 20–21.5 h MLT around 15° N in geomagnetic latitude at an altitude of 450–700 km. Some density depletions correspond to the enhanced ROTI regions related to the EPBs. An electric field enhancement was also observed by the Arase satellite when it passed through one of the density depletion regions at ~20.5 h MLT. The maximum amplitude of the upward velocity to the ground was ~675.1 m/s. The ionospheric virtual height (h’F) at El Arenosillo (37.1° N, 353.3° E) showed an increase from 250 km at 19:15 UT to 310 km at 19:50 UT. The timing when the h’F increased (19:15 UT) corresponded to that of an increase in the solar wind dynamic pressure from 10 nPa to 20 nPa, while the IMF Bz already directed southward around 17:30 UT. The background eastward electric field was estimated to be 1.39 mV/m during the geomagnetic storm on the basis of the ionosonde data at El Arenosillo.
On the other hand, we use the three-dimensional high-resolution bubble model to clarify how the storm-time EPBs expand from the magnetic equator to the mid-latitudes. The ionospheric electric field data over the magnetic equator were needed for the three-dimensional high-resolution bubble model, but the observational data of the ionospheric electric field over the magnetic equator were not available in this event. In this analysis, we also use the GAIA model to reproduce the latitudinal profile of the eastward electric field at the European–African longitudinal sector during the geomagnetic storm. The eastward electric field in the European–African longitudinal sector calculated by the GAIA model showed the enhancement at all latitudes after 19:15 UT. The result was consistent with the observation result obtained by the ionosonde. The amplitude of the calculated eastward electric field during the geomagnetic storm was ~7–8 mV/m near the magnetic equator at 19:45 UT.
The analysis results described above strongly suggests that the eastward electric field enhancement in this event could be caused by the enhancement of the penetration electric field due to the increase of the dynamic pressure under the southward IMF condition. We will discuss in detail the possible generation mechanism of the storm-time EPBs extending to the mid-latitudes based on the simulation results.