Shock fronts, electron-ion equilibration and ICM transport processes in the merging cluster Abell 2146

TL;DR

This study uses deep Chandra X-ray observations of Abell 2146 to analyze shock fronts, electron-ion equilibration, and transport processes in the ICM during a galaxy cluster merger, revealing detailed shock structures and suppressed transport mechanisms.

Contribution

It provides the first detailed measurements of shock widths and electron temperature profiles behind shocks in Abell 2146, offering insights into ICM transport suppression and electron-ion equilibration timescales.

Findings

Shock fronts are remarkably narrow compared to mean free path.

Electron temperature profiles support Coulomb collisional equilibration behind the bow shock.

Transport processes like conduction are strongly suppressed, likely due to magnetic draping.

Abstract

We present a new 400 ks Chandra X-ray observation of the merging galaxy cluster Abell 2146. This deep observation reveals detailed structure associated with the major merger event including the Mach M=2.3+/-0.2 bow shock ahead of the dense, ram pressure stripped subcluster core and the first known example of an upstream shock in the ICM (M=1.6+/-0.1). By measuring the electron temperature profile behind each shock front, we determine the timescale for the electron population to thermally equilibrate with the shock-heated ions. We find that the temperature profile behind the bow shock is consistent with the timescale for Coulomb collisional equilibration and the postshock temperature is lower than expected for instant shock-heating of the electrons. Although like the Bullet cluster the electron temperatures behind the upstream shock front are hotter than expected, favouring the instant heating model, the uncertainty on the temperature values is greater here and there is significant substructure complicating the interpretation. We also measured the width of each shock front and the contact discontinuity on the leading edge of the subcluster core to investigate the suppression of transport processes in the ICM. The upstream shock is ~440 kpc in length but appears remarkably narrow over this distance with a best-fit width of only 6^{+5}_{-3} kpc compared with the mean free path of 23+/-5 kpc. The leading edge of the subcluster core is also narrow with an upper limit on the width of only 2 kpc separating the cool, multiphase gas at 0.5-2 keV from the shock-heated surrounding ICM at ~6 keV. The strong suppression of diffusion and conduction across this edge suggests a magnetic draping layer may have formed around the subcluster core.[abridged]