4.7 Article

The effect of baryons on the inner density profiles of rich clusters

期刊

出版社

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stv1341

关键词

galaxies: clusters: general; galaxies: haloes; cosmology: theory; dark matter

资金

  1. Science and Technology Facilities Council [ST/F001166/1]
  2. Dutch National Computing Facilities Foundation (NCF)
  3. Netherlands Organization for Scientific Research (NWO)
  4. European Research Council under European Union/ERC [278594-GasAroundGalaxies, GA 267291, GA 238356]
  5. Belgian Science Policy Office [AP P7/08 CHARM]
  6. BIS National E-infrastructure capital grant [ST/K00042X/1]
  7. STFC [ST/H008519/1]
  8. STFC DiRAC [ST/K003267/1]
  9. Durham University
  10. PRACE
  11. Science and Technology Facilities Council [ST/H008519/1, ST/I00162X/1, ST/L00061X/1, ST/M007006/1, ST/K00042X/1, ST/L00075X/1] Funding Source: researchfish
  12. STFC [ST/I00162X/1, ST/I004459/1, ST/L00061X/1, ST/K00042X/1, ST/I004459/2, ST/L00075X/1, ST/H008519/1, ST/M007006/1] Funding Source: UKRI

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We use the 'Evolution and assembly of galaxies and their environments' (EAGLE) cosmological simulation to investigate the effect of baryons on the density profiles of rich galaxy clusters. We focus on EAGLE clusters with M-200 > 10(14) M-circle dot of which we have six examples. The central brightest cluster galaxies (BCGs) in the simulation have steep stellar density profiles, rho(*) (r) proportional to. r(-3). Stars dominate the mass density for r < 10 kpc, and, as a result, the total mass density profiles are steeper than the Navarro-Frenk-White (NFW) profile, in remarkable agreement with observations. The dark matter halo itself closely follows the NFW form at all resolved radii (r greater than or similar to 3.0 kpc). The EAGLE BCGs have similar surface brightness and line-of-sight velocity dispersion profiles as the BCGs in the sample of Newman et al., which have the most detailed measurements currently available. After subtracting the contribution of the stars to the central density, Newman et al. infer significantly shallower slopes than the NFW value, in contradiction with the EAGLE results. We discuss possible reasons for this discrepancy, and conclude that an inconsistency between the kinematical model adopted by Newman et al. for their BCGs, which assumes isotropic stellar orbits, and the kinematical structure of the EAGLE BCGs, in which the orbital stellar anisotropy varies with radius and tends to be radially biased, could explain at least part of the discrepancy.

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