Abstract

Radio relics are diffuse synchrotron sources that illuminate shock waves in the intracluster medium. In recent years, radio telescopes have provided detailed observations about relics. Consequently, cosmological simulations of radio relics need to provide a similar amount of detail. In this methodological work, we include information on adiabatic compression and expansion, which have been neglected in the past in the modelling of relics. In a cosmological simulation of a merging galaxy cluster, we follow the energy spectra of shock accelerated cosmic-ray electrons using Lagrangian tracer particles. On board of each tracer particle, we compute the temporal evolution of the energy spectrum under the influence of synchrotron radiation, inverse Compton scattering, and adiabatic compression and expansion. Exploratory tests show that the total radio power and, hence, the integrated radio spectrum are not sensitive to the adiabatic processes. This is attributed to small changes in the compression ratio over time.

Highlights

  • Radio relics are diffuse radio sources observed at the periphery of galaxy clusters

  • The inclusion of adiabatic processes might be relevant, when studying the filamentary structures observed in several relics

  • The filamentary structures evolve on timescales that are shorter than the cooling times

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Summary

Introduction

Radio relics are diffuse radio sources observed at the periphery of galaxy clusters. Relics are the manifestations of cosmic-ray electrons being "shock accelerated" to high energies [1,2,3]. The shock waves develop naturally in the intracluster medium (ICM) during cluster mergers and the accretion of matter. These shock waves (re-) accelerate the ICM electrons to high energies via diffusive shock acceleration (DSA) [4,5]. High-resolution observations show that relics are non-uniform structures and they show threads and filaments on kpc-scales [6,7]. The origin of these filaments is still unknown. They might trace magnetic filaments, the underlying gas density, or the Mach number distribution of the shock wave

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