4.7 Article

The structure of cluster merger shocks: turbulent width and the electron heating time-scale

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 514, Issue 1, Pages 1477-1493

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stac1055

Keywords

galaxies: clusters: individual: Abell2146; intergalactic medium; X-rays: galaxies: clusters

Funding

  1. STFC Ernest Rutherford Fellowship
  2. Anne McLaren Fellowship
  3. National Aeronautics and Space Administration [GO8-19110A, G08-19110B, G08-19110C, G08-19110D]
  4. National Aeronautics Space Administration [NAS8-03060]
  5. Gates Cambridge Scholarship
  6. St John's College Benefactors' Scholarships
  7. NSERC (Natural Sciences and Engineering Research Council of Canada) through the Postgraduate Scholarship-Doctoral Program (PGS D) [PGSD3-535124-2019]
  8. FRQNT (Fonds de recherche du Quebec - Nature et technologies) through the FRQNT Graduate Studies Research Scholarship [274532]

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This study presents observations and measurements of shock widths during a cluster merger process, revealing that narrow collisionless shocks can appear broader in projection due to local gas motions. The research also measures the time scale for electron and ion thermal equilibration and finds no evidence of electron heating beyond adiabatic compression in these cluster merger shocks.
We present a new 2 Ms Chandra observation of the cluster merger Abell 2146, which hosts two huge M similar to 2 shock fronts each similar to 500 kpc across. For the first time, we resolve and measure the width of cluster merger shocks. The best-fitting width for the bow shock is 17 +/- 1 kpc and for the upstream shock is 10.7 +/- 0.3 kpc. A narrow collisionless shock will appear broader in projection if its smooth shape is warped by local gas motions. We show that both shock widths are consistent with collisionless shocks blurred by local gas motions of 290 +/- 30 km s(-1). The upstream shock forms later on in the merger than the bow shock and is therefore expected to be significantly narrower. From the electron temperature profile behind the bow shock, we measure the time-scale for the electrons and ions to come back into thermal equilibrium. We rule out rapid thermal equilibration of the electrons with the shock-heated ions at the 6a level. The observed temperature profile instead favours collisional equilibration. For these cluster merger shocks, which have low sonic Mach numbers and propagate through a high beta plasma, we find no evidence for electron heating over that produced by adiabatic compression. Our findings are expected to be valid for collisionless shocks with similar parameters in other environments and support the existing picture from the solar wind and supernova remnants. The upstream shock is consistent with this result but has a more complex structure, including a similar to 2 keV increase in temperature similar to 50 kpc ahead of the shock.

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