Quantifying the Magnetic Structure of a Coronal Shock Producing a Type II Radio Burst

Type II radio bursts are thought to be produced by shock waves in the solar atmosphere. However, what magnetic conditions are needed for the generation of type II radio bursts is still a puzzling issue. Here, we quantify the magnetic structure of a coronal shock associated with a type II radio burst...

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Published inThe Astrophysical journal Vol. 929; no. 2; pp. 175 - 187
Main Authors Su, W., Li, T. M., Cheng, X., Feng, L., Zhang, P. J., Chen, P. F., Ding, M. D., Chen, L. J., Guo, Y., Wang, Y., Li, D., Zhang, L. Y.
Format Journal Article
LanguageEnglish
Published The American Astronomical Society 01.04.2022
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ISSN0004-637X
1538-4357
DOI10.3847/1538-4357/ac5fac

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Abstract Type II radio bursts are thought to be produced by shock waves in the solar atmosphere. However, what magnetic conditions are needed for the generation of type II radio bursts is still a puzzling issue. Here, we quantify the magnetic structure of a coronal shock associated with a type II radio burst. Based on multiperspective extreme-ultraviolet observations, we reconstruct the three-dimensional (3D) shock surface. By using a magnetic field extrapolation model, we then derive the orientation of the magnetic field relative to the normal of the shock front ( θ Bn ) and the Alfvén Mach number ( M A ) on the shock front. Combining the radio observations from the Nancay Radio Heliograph, we obtain the source region of the type II radio burst on the shock front. It is found that the radio burst is generated by a shock with M A ≳ 1.5 and a bimodal distribution of θ Bn . We also use the Rankine–Hugoniot relations to quantify the properties of the shock downstream. Our results provide a quantitative 3D magnetic structure condition of a coronal shock that produces a type II radio burst.
AbstractList Type II radio bursts are thought to be produced by shock waves in the solar atmosphere. However, what magnetic conditions are needed for the generation of type II radio bursts is still a puzzling issue. Here, we quantify the magnetic structure of a coronal shock associated with a type II radio burst. Based on multiperspective extreme-ultraviolet observations, we reconstruct the three-dimensional (3D) shock surface. By using a magnetic field extrapolation model, we then derive the orientation of the magnetic field relative to the normal of the shock front ( θ Bn ) and the Alfvén Mach number ( M A ) on the shock front. Combining the radio observations from the Nancay Radio Heliograph, we obtain the source region of the type II radio burst on the shock front. It is found that the radio burst is generated by a shock with M A ≳ 1.5 and a bimodal distribution of θ Bn . We also use the Rankine–Hugoniot relations to quantify the properties of the shock downstream. Our results provide a quantitative 3D magnetic structure condition of a coronal shock that produces a type II radio burst.
Author Zhang, L. Y.
Feng, L.
Chen, P. F.
Chen, L. J.
Li, D.
Li, T. M.
Ding, M. D.
Guo, Y.
Su, W.
Wang, Y.
Zhang, P. J.
Cheng, X.
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Snippet Type II radio bursts are thought to be produced by shock waves in the solar atmosphere. However, what magnetic conditions are needed for the generation of type...
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StartPage 175
SubjectTerms Shocks
Solar coronal mass ejection shocks
Title Quantifying the Magnetic Structure of a Coronal Shock Producing a Type II Radio Burst
URI https://iopscience.iop.org/article/10.3847/1538-4357/ac5fac
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