Abstract

Shock ripples are ion-inertial-scale waves propagating within the front region of magnetized quasi-perpendicular collisionless shocks. The ripples are thought to influence particle dynamics and acceleration at shocks. With the four magnetospheric multiscale (MMS) spacecraft, it is for the first time possible to fully resolve the small scale ripples in space. We use observations of one slow crossing of the Earth’s non-stationary bow shock by MMS. From multi-spacecraft measurements we show that the non-stationarity is due to ripples propagating along the shock surface. We find that the ripples are near linearly polarized waves propagating in the coplanarity plane with a phase speed equal to the local Alfvén speed and have a wavelength close to 5 times the upstream ion inertial length. The dispersive properties of the ripples resemble those of Alfvén ion cyclotron waves in linear theory. Taking advantage of the slow crossing by the four MMS spacecraft, we map the shock-reflected ions as a function of ripple phase and distance from the shock. We find that ions are preferentially reflected in regions of the wave with magnetic field stronger than the average overshoot field, while in the regions of lower magnetic field, ions penetrate the shock to the downstream region.

Highlights

  • We find that ions are preferentially reflected in regions of the wave with magnetic field stronger than the average overshoot field, while in the regions of lower magnetic field, ions penetrate the shock to the downstream region

  • The goal of this paper is to study the physical properties of the shock ripples

  • Since this partial shock crossing is slow, magnetospheric multiscale (MMS) observes many ripple periods, which allows for detailed analysis of fluctuations and their impact on ion dynamics and reflection

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Summary

Introduction

A distinctly different type of large-amplitude fluctuations in the shock observed in fully kinetic 2D simulations is a whistler branch wave that propagates obliquely to the magnetic field (Hellinger et al 2007, Lembège et al 2009) These waves are different from the previously observed shock ripples and are likely a competing mechanism for shock non-stationarity. In 3D hybrid simulations Burgess et al (2016) found that the shock structure is dominated by a combination of fluctuations propagating along the magnetic field and in the direction of reflected ion gyration. With the observations we characterize in detail the dispersive properties of the ripples and their impact on ion reflection at the shock

The event
The non-stationary shock
Ion reflection off a rippled shock
Discussion
Conclusions
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