Abstract

Electron acceleration to non-thermal energies in low Mach number (M<5) shocks is revealed by radio and X-ray observations of galaxy clusters and solar flares, but the electron acceleration mechanism remains poorly understood. Diffusive shock acceleration, also known as first-order Fermi acceleration, cannot be directly invoked to explain the acceleration of electrons. Rather, an additional mechanism is required to pre-accelerate the electrons from thermal to supra-thermal energies, so they can then participate in the Fermi process. In this work, we use two- and three-dimensional particle-in-cell plasma simulations to study electron acceleration in low Mach number shocks. We focus on the particle energy spectra and the acceleration mechanism in a reference run with M=3 and a quasi-perpendicular pre-shock magnetic field. We find that about 15 percent of the electrons can be efficiently accelerated, forming a non-thermal power-law tail in the energy spectrum with a slope of p~2.4. Initially, thermal electrons are energized at the shock front via shock drift acceleration. The accelerated electrons are then reflected back upstream, where their interaction with the incoming flow generates magnetic waves. In turn, the waves scatter the electrons propagating upstream back toward the shock, for further energization via shock drift acceleration. In summary, the self-generated waves allow for repeated cycles of shock drift acceleration, similarly to a sustained Fermi-like process. This mechanism offers a natural solution to the conflict between the bright radio synchrotron emission observed from the outskirts of galaxy clusters and the low electron acceleration efficiency usually expected in low Mach number shocks.

Highlights

  • Collisionless shocks occur in a wide variety of astrophysical settings: Earth’s bow shock and the solar wind termination shock, supernova remnant (SNR) shocks in the interstellar medium, and structure formation shocks in the intracluster medium (ICM)

  • We find that most of the shock physics is well captured by 2D simulations, when the field is lying in the simulation plane, i.e., φB = 0◦

  • We study from first principles the physics of electron acceleration in a low Mach number (Ms = 3) shock, by means of fully kinetic PIC plasma simulations

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Summary

INTRODUCTION

Collisionless shocks occur in a wide variety of astrophysical settings: Earth’s bow shock and the solar wind termination shock, supernova remnant (SNR) shocks in the interstellar medium, and structure formation shocks in the intracluster medium (ICM). The injection mechanism is expected to be different because the Buneman instability, essential for trapping the electrons near the shock for the SSA process, cannot be triggered at low Mach numbers(Matsumoto et al 2012). The 1D nature of the simulations of Matsukiyo et al (2011) prohibits a self-consistent study of self-generated waves in the upstream, since the wave-vector is confined to be perpendicular to the shock plane Their results certainly suggest that SDA could be a potential injection mechanism, but they have no direct evidence of electron Fermi acceleration. We study electron acceleration in low Mach number shocks using fully kinetic two-dimensional (2D) and three-dimensional (3D) PIC simulations. 2014, in preparation) we will study in detail the nature of the upstream waves and explore the parameter dependence of the electron energy spectrum and acceleration mechanism

SIMULATION SETUP
SHOCK STRUCTURE
PARTICLE ENERGY SPECTRA AND ACCELERATION MECHANISM
Spectral Evolution
The Acceleration Process
Shock Drift Acceleration Theory
Verification of SDA in the Simulation
Fermi Acceleration
Findings
SUMMARY AND DISCUSSION
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