Abstract

At the Earth's low-latitude magnetopause, the Kelvin–Helmholtz instability (KHI), driven by the velocity shear between the magnetosheath and magnetosphere, has been frequently observed during northward interplanetary magnetic field (IMF) periods. However, the signatures of the KHI have been much less frequently observed during southward IMF periods, and how the KHI develops under southward IMF has been less explored. Here, we performed a series of realistic 2D and 3D fully kinetic simulations of a KH wave event observed by the Magnetospheric Multiscale (MMS) mission at the dusk-flank magnetopause during southward IMF on September 23, 2017. The simulations demonstrate that the primary KHI bends the magnetopause current layer and excites the Rayleigh–Taylor instability (RTI), leading to penetration of high-density arms into the magnetospheric side. This arm penetration disturbs the structures of the vortex layer and produces intermittent and irregular variations of the surface waves which significantly reduces the observational probability of the periodic KH waves. The simulations further demonstrate that in the non-linear growth phase of the primary KHI, the lower-hybrid drift instability (LHDI) is induced near the edge of the primary vortices and contributes to an efficient plasma mixing across the magnetopause. The signatures of the large-scale surface waves by the KHI/RTI and the small-scale fluctuations by the LHDI are reasonably consistent with the MMS observations. These results indicate that the multi-scale evolution of the magnetopause KH waves and the resulting plasma transport and mixing as seen in the simulations may occur during southward IMF.

Highlights

  • The Kelvin–Helmholtz instability (KHI) becomes unstable when the plasma shear flow is super-Alfvenic for the magnetic field component parallel to the shear flow (Chandrasekhar, 1961)

  • Clear vortexinduced reconnection (VIR) signatures as reported in the above Magnetospheric Multiscale (MMS) observation events for the northward interplanetary magnetic field (IMF) were not found in this event, the high-time-resolution measurements of MMS frequently detected small-scale fluctuations, which can be interpreted as being generated by the lower-hybrid drift instability (LHDI), excited near the edge of the surface waves

  • We have performed a series of 2D and 3D fully kinetic simulations of an MMS observation event on September 23, 2017 in which the KH waves were observed at the dusk-flank magnetopause during southward IMF

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Summary

INTRODUCTION

The Kelvin–Helmholtz instability (KHI) becomes unstable when the plasma shear flow is super-Alfvenic for the magnetic field component parallel to the shear flow (Chandrasekhar, 1961). A recent three-dimensional (3D) fully kinetic simulation under pure southward IMF conditions demonstrated that strong evolution of magnetic reconnection across thin current layers formed within the KH waves quickly destroys the wave and vortex structures (Nakamura et al, 2020a) This reconnection-driven decay process of the KH vortex may explain the intermittent and irregular variations of the observed KH vortices as well as the low observational probability of the periodic KH waves/vortices during southward IMF. Clear VIR signatures as reported in the above MMS observation events for the northward IMF were not found in this event, the high-time-resolution measurements of MMS frequently detected small-scale fluctuations, which can be interpreted as being generated by the lower-hybrid drift instability (LHDI), excited near the edge of the surface waves To investigate this event in more detail, in the present paper, we perform a series of 2D and 3D fully kinetic simulations with parameters matched to this MMS event. V, we summarize the results and discuss differences in the evolution of the KH waves between the northward and southward IMF conditions

Simulation settings
Initial equilibrium
Overview of the simulation results
Secondary RTI
Turbulent reconnection
Plasma transport and mixing
Detection probability of the primary KH mode
Summary
IMF dependence
Some remarks on future work
Findings
CONCLUSIONS
Full Text
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