EVOLUTION OF THE GALAXY-DARK MATTER CONNECTION AND THE ASSEMBLY OF GALAXIES IN DARK MATTER HALOS

We present a new model to describe the galaxy-dark matter connection across cosmic time, which unlike the popular subhalo abundance-matching technique is self-consistent in that it takes account of the facts that (1) subhalos are accreted at different times and (2) the properties of satellite galaxies may evolve after accretion. Using observations of galaxy stellar mass functions (SMFs) out to z ~ 4, the conditional SMF at z ~ 0.1 obtained from Sloan Digital Sky Survey galaxy group catalogs, and the two-point correlation function (2PCF) of galaxies at z ~ 0.1 as a function of stellar mass, we constrain the relation between galaxies and dark matter halos over the entire cosmic history from z ~ 4 to the present. This relation is then used to predict the median assembly histories of different stellar mass components within dark matter halos (central galaxies, satellite galaxies, and halo stars). We also make predictions for the 2PCFs of high-z galaxies as function of stellar mass. Our main findings are the following: (1) Our model reasonably fits all data within the observational uncertainties, indicating that the [LAMBDA]CDM concordance cosmology is consistent with a wide variety of data regarding the galaxy population across cosmic time. (2) At low-z, the stellar mass of central galaxies increases with halo mass as M super(0.3) and M super([> ~]4.0) at the massive and low-mass ends, respectively. The ratio M[low *],c/M reveals a maximum of ~0.03 at a halo mass M ~ 10 super(11.8) h super(-1) M sub([middot in circle]), much lower than the universal baryon fraction (~0.17). At higher redshifts the maximum in M[low *],c/M remains close to ~0.03, but shifts to higher halo mass. (3) The inferred timescale for the disruption of satellite galaxies is about the same as the dynamical friction timescale of their subhalos. (4) The stellar mass assembly history of central galaxies is completely decoupled from the assembly history of its host halo; the ratio M[low *],c/M initially increases rapidly with time until the halo mass reaches ~10 super(12) h super(-1) M sub([middot in circle]), at which point M[low *],c/M ~ 0.03. Once M [> ~]10 super(12) h super(-1) M sub([middot in circle]), there is little growth in M[low *],c, causing the ratio M[low *],c/M to decline. In Milky Way (MW)-sized halos more than half of the central stellar mass is assembled at z [