• DOI:10.3847/1538-4357/ac1acd
• Corpus ID: 236740875

Observations of Shock Propagation through Turbulent Plasma in the Solar Corona

@article{Carley2021ObservationsOS,
  title={Observations of Shock Propagation through Turbulent Plasma in the Solar Corona},
  author={Eoin P. Carley and Baptiste Cecconi and Hamish A. S. Reid and Carine Briand and K. Sasikumar Raja and Sophie Masson and Vladimir Dorovskyy and Caterina Tiburzi and Nicole Vilmer and Pietro Zucca and Philippe Zarka and Michel Tagger and Jean-Mathias Grie{\ss}meier and St{\'e}phane Corbel and Gilles Theureau and Alan Loh and Julien N. Girard},
  journal={The Astrophysical Journal},
  year={2021},
  volume={921}
}

• E. Carley, B. Cecconi, +14 authors J. Girard
• Published 3 March 2021
• Physics
• The Astrophysical Journal

Eruptive activity in the solar corona can often lead to the propagation of shock waves. In the radio domain the primary signature of such shocks are type II radio bursts, observed in dynamic spectra as bands of emission slowly drifting toward lower frequencies over time. These radio bursts can sometimes have an inhomogeneous and fragmented fine structure, but the cause of this fine structure is currently unclear. Here we observe a type II radio burst on 2019 March 20th using the New Extension in Nançay Upgrading LOFAR, a radio interferometer observing between 10–85 MHz. We show that the distribution of size scales of density perturbations associated with the type II fine structure follows a power law with a spectral index in the range of α = −1.7 to −2.0, which closely matches the value of −5/3 expected of fully developed turbulence. We determine this turbulence to be upstream of the shock, in background coronal plasma at a heliocentric distance of ∼2 R ⊙. The observed inertial size scales of the turbulent density inhomogeneities range from ∼62 Mm to ∼209 km. This shows that type II fine structure and fragmentation can be due to shock propagation through an inhomogeneous and turbulent coronal plasma, and we discuss the implications of this on electron acceleration in the coronal shock.