4.7 Article

EVOLUTION OF THE MERGER-INDUCED HYDROSTATIC MASS BIAS IN GALAXY CLUSTERS

Journal

ASTROPHYSICAL JOURNAL
Volume 751, Issue 2, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.1088/0004-637X/751/2/121

Keywords

cosmology: theory; galaxies: clusters: general

Funding

  1. NSF [AST-1009811, OCI-0904484]
  2. NASA ATP [NNX11AE07G]
  3. Direct For Computer & Info Scie & Enginr
  4. Office of Advanced Cyberinfrastructure (OAC) [0904484] Funding Source: National Science Foundation
  5. Division Of Astronomical Sciences
  6. Direct For Mathematical & Physical Scien [1009811] Funding Source: National Science Foundation

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In this work, we examine the effects of mergers on the hydrostatic mass estimate of galaxy clusters using high-resolution Eulerian cosmological simulations. We utilize merger trees to isolate the last merger for each cluster in our sample and follow the time evolution of the hydrostatic mass bias as the systems relax. We find that during a merger, a shock propagates outward from the parent cluster, resulting in an overestimate in the hydrostatic mass bias. After the merger, as a cluster relaxes, the bias in hydrostatic mass estimate decreases but remains at a level of -5%-10% with 15%-20% scatter within r(500). We also investigate the post-merger evolution of the pressure support from bulk motions, a dominant cause of this residual mass bias. At r(500), the contribution from random motions peaks at 30% of the total pressure during the merger and quickly decays to similar to 10%-15% as a cluster relaxes. Additionally, we use a measure of the random motion pressure to correct the hydrostatic mass estimate. We discover that 4 Gyr after mergers, the direct effects of the merger event on the hydrostatic mass bias have become negligible. Thereafter, the mass bias is primarily due to residual bulk motions in the gas which are not accounted for in the hydrostatic equilibrium equation. We present a hydrostatic mass bias correction method that can recover the unbiased cluster mass for relaxed clusters with 9% scatter at r(500) and 11% scatter in the outskirts, within r(200).

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