4.7 Article

Baryon content of massive galaxy clusters at 0.57 < z < 1.33

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 455, Issue 1, Pages 258-275

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stv2303

Keywords

Galaxy: evolution; galaxies: clusters: general; large-scale structure of Universe; X-rays: galaxies: clusters

Funding

  1. VLT programmes [088.A-0889, 089.A-0824]
  2. DFG Cluster of Excellence 'Origin and Structure of the Universe'
  3. Transregio programme TR33 'The Dark Universe'
  4. Fermi Research Alliance, LLC [De-AC02-07CH11359]
  5. United States Department of Energy
  6. NSF [AST-1009012, AST-1009649, MRI-0723073]
  7. German Federal Ministry of Economics and Technology (BMWi) [50 OR 1210]
  8. National Science Foundation [ANT-0638937]
  9. NSF Physics Frontier Center [PHY-0114422]
  10. Kavli Foundation
  11. Gordon and Betty Moore Foundation
  12. [C18-12246]
  13. [C19-12447]
  14. [60099]
  15. [70053]
  16. [80012]
  17. Office of Polar Programs (OPP) [1248097] Funding Source: National Science Foundation

Ask authors/readers for more resources

We study the stellar, brightest cluster galaxy (BCG) and intracluster medium (ICM) masses of 14 South Pole Telescope (SPT) selected galaxy clusters with median redshift z = 0.9 and mass M-500 = 6 x 10(14) M-circle dot. We estimate stellar masses for each cluster and BCG using six photometric bands, the ICM mass using X-ray observations and the virial masses using the SPT Sunyaev-Zel'dovich effect signature. At z = 0.9, the BCG mass M-*(BCG) constitutes 0.12 +/- 0.01 per cent of the halo mass for a 6 x 10(14) M-circle dot cluster, and this fraction falls as M-500(-0.58 +/- 0.07). The cluster stellar mass function has a characteristic mass M-0 = 10(11.0 +/- 0.1) M-circle dot, and the number of galaxies per unit mass in clusters is larger than in the field by a factor of 1.65 +/- 0.20. We combine our SPT sample with previously published samples at low redshift and correct to a common initial mass function and for systematic virial mass differences. We then explore mass and redshift trends in the stellar fraction f(*), the ICM fraction f(ICM), the collapsed baryon fraction f(c) and the baryon fraction f(b). At a pivot mass of 6 x 10(14) M-circle dot and redshift z = 0.9, the characteristic values are f(*) = 1.1 +/- 0.1 per cent, f(ICM) = 9.6 +/- 0.5 per cent, f(c) = 10.7 +/- 1.1 per cent and f(b) = 10.7 +/- 0.6 per cent. These fractions all vary with cluster mass at high significance, with higher mass clusters having lower f(*) and f(c) and higher f(ICM) and f(b). When accounting for a 15 per cent systematic virial mass uncertainty, there is no statistically significant redshift trend at fixed mass. Our results support the scenario where clusters grow through accretion from subclusters (higher f(*), lower f(ICM)) and the field (lower f(*), higher f(ICM)), balancing to keep f(*) and f(ICM) approximately constant since z similar to 0.9.

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