Overexpansion-dominated coronal mass ejection formation and induced radio bursts

被引:3
|
作者
Wang, B. T. [1 ,2 ]
Cheng, X. [1 ,2 ,3 ]
Song, H. Q. [4 ,5 ]
Ding, M. D. [1 ,2 ]
机构
[1] Nanjing Univ, Sch Astron & Space Sci, Nanjing 210023, Peoples R China
[2] Nanjing Univ, Minist Educ, Key Lab Modern Astron & Astrophys, Nanjing 210093, Peoples R China
[3] Max Planck Inst Solar Syst Res, D-37077 Gottingen, Germany
[4] Shandong Univ, Shandong Prov Key Lab Opt Astron & Solar Terr Env, Weihai 264209, Shandong, Peoples R China
[5] Shandong Univ, Inst Space Sci, Weihai 264209, Shandong, Peoples R China
基金
国家重点研发计划;
关键词
Sun: corona; Sun: coronal mass ejections; Sun: flares; MAGNETIC RECONNECTION; KINEMATIC EVOLUTION; ELECTRON EVENTS; HIGH-CADENCE; ACCELERATION; WAVE; FLARES; PROMINENCE; RELEASE; GENESIS;
D O I
10.1051/0004-6361/202244275
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Aims. Coronal mass ejections (CMEs) are the most fascinating explosions in the Solar System. Their formation is still not fully understood, however. Methods. We investigated a well-observed CME on 2021 May 7 that showed a typical three-component structure and was continuously observed from 0 to 3 R-circle dot by a combination of SDO/AIA (0-1.3 R-circle dot), PROBA2/SWAP (0-1.7 R-circle dot), and MLSO/K-Cor (1.05-3 R-circle dot). Furthermore, we compared the morphological discrepancy between the CME white-light bright core and the extreme-UV (EUV) blob. We finally explored the origin of various radio bursts that are closely related to the interaction of the CME overexpansion with a nearby streamer. Results. An interesting finding is that the height increases of the CME leading front and of the bright core are dominated by the overexpansion during the CME formation. The aspect ratios of the CME bubble and bright core, quantifying the overexpansion, are found to decrease as the SO/STIX 4-10 keV and GOES 1-8 angstrom soft X-ray flux of the associated flare increases near the peaks. This indicates that the flare reconnection plays an important role in the first overexpansion. The CME bubble even undergoes a second overexpansion, although it is relatively weak, which is closely related to the compression with a nearby streamer and likely arises from an ideal magnetohydrodynamics process. Moreover, the CME EUV blob is found to be relatively lower and wider than the CME white-light bright core, which may correspond to the bottom part of the growing CME flux rope. The interaction between the CME and the streamer leads to two type II radio bursts, one that is drifting normally and another that is stationary, which are speculated to be induced by two different sources of the CME-driven shock front. The bidirectional electrons shown in series of C-shaped type III bursts suggest that the interchange reconnection is also involved during the interaction of the CME and streamer.
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页数:8
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