Help Privacy Policy Disclaimer
  Advanced SearchBrowse




Journal Article

Three-dimensional Magnetic and Thermodynamic Structures of Solar Microflares


Cheng,  X.
Department Sun and Heliosphere, Max Planck Institute for Solar System Research, Max Planck Society;

Fulltext (restricted access)
There are currently no full texts shared for your IP range.
Fulltext (public)
There are no public fulltexts stored in PuRe
Supplementary Material (public)
There is no public supplementary material available

Li, Z. F., Cheng, X., Chen, F., Chen, J., & Ding, M. D. (2022). Three-dimensional Magnetic and Thermodynamic Structures of Solar Microflares. The Astrophysical Journal, 930, L7. doi:10.3847/2041-8213/ac67aa.

Cite as: https://hdl.handle.net/21.11116/0000-000D-BD11-B
Microflares, one of the small-scale solar activities, are believed to be caused by magnetic reconnection. Nevertheless, their three-dimensional (3D) magnetic structures, thermodynamic structures, and physical links to reconnection are unclear. In this Letter, based on a high-resolution 3D radiative magnetohydrodynamic simulation of the quiet Sun spanning from the upper convection zone to the corona, we investigate the 3D magnetic and thermodynamic structures of three homologous microflares. It is found that they originate from localized hot plasma embedded in the chromospheric environment at the height of 2-10 Mm above the photosphere and last for 3-10 minutes with released magnetic energy in the range of 1027-1028 erg. The heated plasma is almost cospatial with the regions where the heating rate per particle is maximal. The 3D velocity field reveals a pair of converging flows with velocities of tens of km s-1 moving toward and outflows with velocities of about 100 km s-1 moving away from the hot plasma. These features support magnetic reconnection playing a critical role in heating the localized chromospheric plasma to coronal temperature, giving rise to the observed microflares. The magnetic topology analysis further discloses that the reconnection region is located near quasi-separators where both current density and squashing factors are maximal although the specific topology may vary from a tether-cutting to fan-spine-like structure.