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A new approach to the maser emission in the solar corona View all abstracts by submitter

Stephane Regnier   Submitted: 2015-08-25 03:06

The electron plasma frequency ω_pe and electron gyrofrequency Omega_e are two parameters that allow us to describe the properties of a plasma and to constrain the physical phenomena at play, for instance, whether a maser instability develops. In this paper, we aim to show that the maser instability can exist in the solar corona. We perform an in-depth analysis of the ω_pe/Omega_e ratio for simple theoretical and complex solar magnetic field configurations. Using the combination of force-free models for the magnetic field and hydrostatic models for the plasma properties, we determine the ratio of the plasma frequency to the gyrofrequency for electrons. For the sake of comparison, we compute the ratio for bipolar magnetic fields containing a twisted flux bundle, and for four different observed active regions. We also study how ω_pe/Omega_e is affected by the potential and non-linear force-free field models. We demonstrate that the ratio of the plasma frequency to the gyrofrequency for electrons can be estimated by this novel method combining magnetic field extrapolation techniques and hydrodynamic models. Even if statistically not significant, values of ω_pe/Omega_e ≤ 1 are present in all examples, and are located in the low corona near to photosphere below one pressure scale-height and/or in the vicinity of twisted flux bundles. The values of ω_pe/Omega_e are lower for non-linear force-free fields than potential fields, thus increasing the possibility of maser instability in the corona. From this new approach for estimating ω_pe/Omega_e, we conclude that the electron maser instability can exist in the solar corona above active regions. The importance of the maser instability in coronal active regions depends on the complexity and topology of the magnetic field configurations.

Authors: S. Regnier
Projects: None

Publication Status: Published in A&A
Last Modified: 2015-08-25 16:46
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