Conditions for electron-cyclotron maser emission in the solar corona

TL;DR

This study explores the conditions under which electron-cyclotron maser emission can occur in the solar corona, focusing on magnetic field strength and plasma density, and suggests ECM as a plausible mechanism for certain high-frequency solar radio bursts.

Contribution

The paper provides observational evidence and maps of the solar corona showing where ECM conditions are met, highlighting the role of magnetic fields and plasma parameters in emission mechanisms.

Findings

ECM conditions are met at heights below 1.07 solar radii in active regions.

Magnetic field strengths greater than 40 G are associated with ECM feasibility.

High Alfvén velocities (> 0.02 c) are found in regions where ECM could occur.

Abstract

Context. The Sun is an active source of radio emission ranging from long duration radio bursts associated with solar flares and coronal mass ejections to more complex, short duration radio bursts such as solar S bursts, radio spikes and fibre bursts. While plasma emission is thought to be the dominant emission mechanism for most radio bursts, the electron-cyclotron maser (ECM) mechanism may be responsible for more complex, short-duration bursts as well as fine structures associated with long-duration bursts. Aims. We investigate the conditions for ECM in the solar corona by considering the ratio of the electron plasma frequency {\omega}p to the electron-cyclotron frequency {\Omega}e. The ECM is theoretically possible when {\omega}p/{\Omega}e < 1. Methods. Two-dimensional electron density, magnetic field, plasma frequency, and electron cyclotron frequency maps of the off- limb corona were created using observations from SDO/AIA and SOHO/LASCO, together with potential field extrapolations of the magnetic field. These maps were then used to calculate {\omega}p/{\Omega}e and Alfven velocity maps of the off-limb corona. Results. We found that the condition for ECM emission ({\omega}p/{\Omega}e < 1) is possible at heights < 1.07 R_sun in an active region near the limb; that is, where magnetic field strengths are > 40 G and electron densities are greater than 3x10^8 cm-3. In addition, we found comparatively high Alfv\'en velocities (> 0.02 c or > 6000 km s-1) at heights < 1.07 R_sun within the active region. Conclusions. This demonstrates that the condition for ECM emission is satisfied within areas of the corona containing large magnetic fields, such as the core of a large active region. Therefore, ECM could be a possible emission mechanism for high-frequency radio and microwave bursts.