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-P33] Ionospheric response to solar flares – how fast does the disturbance propagate?

*Maletckii Boris1Astafyeva Elvira1、Pedatella Nicholas2 (1.Institut de Physique du Globe de Paris, Universite Paris Cite, CNRS、2.NSF National Center for Atmospheric Research, High Altitude Observatory)

キーワード:Ionosphere, Solar Flares, Sudden Ionospheric Disturbance, GNSS, TEC

A Solar Flare (SF) is a tremendous explosion on the Sun that is characterised by the increased radiation in the X-ray and in the ultraviolet (UV), a stream of a wide range of energy particles. Several effects are caused when they come into contact with the atmosphere of the Earth, including Sudden Ionospheric Disturbances (SID), which are a collective term for the quick rise in ionospheric ionization resulting from increased X and UV radiation.
It is generally assumed that the SID occurs instantly and simultaneously on the entire dayside. In this work, we use high-rate 1 sec data of ionospheric total electron content (TEC) from world-wide distributed receivers of the Global Navigation Satellite Systems (GNSS), and we analyze the global dayside TEC response to thirteen solar flares that occurred between 2003 and 2023. The high temporal resolution allowed us, for the first time, to observe the propagation of SID from the subsolar point to the dusk regions. We find that the apparent velocity of SID propagation varies between ~250 and ~500 km/s, and might depend on the position of the flare on the solar disk (on disk and limb, respectively).
In addition, we noted that the apparent SID propagation is anisotropic, i.e., depending on the observation’s location relatively to a sub-solar point. The velocity of the enhancement varies in a different part of dayside of the ionosphere. We performed modelling of SID effects and investigated the possible reasons which can be responsible for this effect, including background level of ionization, solar-zenith angle dependency and thermospheric composition changes.
Figure. The development of SID as seen in TTD of dTEC/dt parameter (left panel) and Global dTEC/dt Maps (right panels) for the 20 September 2023 M8.2 flare.