Dissipative instability in partially ionised prominence plasmas
Istvan Ballai, Ramon Oliver, Marios Alexandrou

TL;DR
This paper analyzes how partial ionisation and viscosity influence dissipative instabilities at the boundary between solar prominences and the corona, revealing conditions under which these instabilities occur.
Contribution
It provides a new analytical framework for understanding dissipative instability in partially ionised prominence plasmas, considering the effects of ionisation degree and viscosity.
Findings
Dissipative instabilities occur at flow speeds below Kelvin-Helmholtz threshold.
Viscosity destabilizes, while partial ionisation stabilizes the interface.
Instability in prominences has very small growth rates, unlikely to cause observed flows.
Abstract
We investigate the nature of dissipative instability at the boundary (seen here as tangential discontinuity) between the viscous corona and the partially ionised prominence plasma in the incompressible limit. The importance of the partial ionisation is investigated in terms of the ionisation fraction. Matching the solutions for the transversal component of the velocity and total pressure at the interface between the prominence and coronal plasmas, we derive a dispersion relation whose imaginary part describes the evolution of the instability. Results are obtained in the limit of weak dissipation. Using simple analytical methods, we show that dissipative instabilities appear for flow speeds that are lower than the Kelvin-Helmholtz instability threshold. While viscosity tends to destabilise the plasma, the effect of partial ionisation (through the Cowling resistivity) will act towards…
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