2005/09/26 by Hideki Yahagi, H. Yahagi, K. Bekki +1 · 2 citations
Physics and Astronomy · #Astronomy and Astrophysical Research #Electrical and Electromagnetic Research #Galaxies: Formation, Evolution, Phenomena #astro-ph
paper · pdf · doi:10.1111/j.1745-3933.2005.00111.x
published as Mon.Not.Roy.Astron.Soc.Lett.364:L86-L90,2005 · 5 pages, 5 figures (color figure for Figure 1), accepted by MNRAS. The dependences of the results on the initial GC density profiles at z=6 are added
arxiv created 2005/09/26 · openalex publication_date 2005/10/28 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/30
We first present the results of numerical simulations on formation processes and physical properties of old globular clusters (GCs) located within clusters of galaxies (‘intracluster GCs’) and in between clusters of galaxies (‘intercluster GCs’). Our high-resolution cosmological simulations with models of GC formation at high redshifts (z > 6) show that about 30 per cent of all GCs in a rich cluster can be regarded as intracluster GCs that can freely drift, being trapped by gravitational potential of the cluster rather than by the cluster member galaxies. The radial surface density profiles of the simulated intracluster GCs are highly likely to be flatter than those of GCs within cluster member galaxies. We also find that about 1 per cent of all GCs formed before z > 6 are not located within any virialized haloes and can be regarded as ‘intercluster’ (or ‘intergalactic’) GCs. We discuss the dependencies of the physical properties of intracluster and intercluster GCs on the initial density profiles of GCs within low-mass dark matter haloes at high redshifts (z > 6).