Abstract

We investigate the evolution of the galaxy stellar mass function at high-redshift ($z\ge 5$) using a pair of large cosmological hydrodynamical simulations: {\em MassiveBlack} and {\em MassiveBlack-II}. By combining these simulations we can study the properties of galaxies with stellar masses greater than $10^{8}\,{\rm M_{\odot}}\,h^{-1}$ and (co-moving) number densities of $\log_{10}(\phi\, [{\rm Mpc^{-3}\,dex^{-1}}\,h^{3}])>-8$. Observational determinations of the galaxy stellar mass function at very-high redshift typically assume a relation between the observed UV luminosity and stellar mass-to-light ratio which is applied to high-redshift samples in order to estimate stellar masses. This relation can also be measured from the simulations. We do this, finding two significant differences with the usual observational assumption: it evolves strongly with redshift and has a different shape. Using this relation to make a consistent comparison between galaxy stellar mass functions we find that at $z=6$ and above the simulation predictions are in good agreement with observed data over the whole mass range. Without using the correct UV luminosity and stellar mass-to-light ratio, the discrepancy would be up to two orders of magnitude for large galaxies $>10^{10}\,{\rm M_{\odot}}\,h^{-1}$. At $z=5$, however the stellar mass function for low mass $<10^{9}\,{\rm M_{\odot}}\,h^{-1}$ galaxies is overpredicted by factors of a few, consistent with the behaviour of the UV luminosity function, and perhaps a sign that feedback in the simulation is not efficient enough for these galaxies.

Highlights

  • The observational exploration of the high-redshift (z > 2) Universe has been driven, over the past 10–15 years, predominantly by deep Hubble Space Telescope (HST) surveys

  • At the high-mass end, we have shown that correcting for the evolution of the relationship between UV luminosity and mass-to-light ratio brings the observations and simulations into agreement, and this would be likely to work for the Jaacks et al results

  • We have investigated the high-redshift (z = 5–10) evolution of the galaxy stellar mass function (GSMF) using a pair of large cosmological hydrodynamic simulations MassiveBlack and MassiveBlack-II

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Summary

INTRODUCTION

The observational exploration of the high-redshift (z > 2) Universe has been driven, over the past 10–15 years, predominantly by deep Hubble Space Telescope (HST) surveys. By combining ACS optical and NICMOS or WFC3 near-IR imaging with Spitzer Infrared Array Camera (IRAC) observations, it becomes possible to probe the rest-frame ultraviolet–optical (UV– optical) spectral energy distributions (SEDs) of galaxies at z = 4−8 (e.g. Eyles et al 2005; Gonzalez et al 2012). We use state-of-the-art cosmological hydrodynamical simulations of structure formation (MassiveBlack and MassiveBlack-II) to investigate their predictions of the GSMF and compare it with current constraints These runs are large, high-resolution simulations, with more than 65.5 billion resolution elements used in a box of roughly cubic gigaparsec scales (for MassiveBlack), making it by far the largest cosmological smooth particle hydrodynamics (SPH) simulation to date with ‘full physics’ of galaxy formation (meaning here an inclusion of radiative cooling, star formation, black hole growth and associated feedback physics) ever carried out. The combination of the two simulations allows us to probe galaxies with stellar masses greater than 108 M h−1 and (comoving) number densities of log10(φ[Mpc−3 dex−1 h3]) > −8, a range well matched with current observations at high redshift.

Simulation runs
THE GALAXY STELLAR MASS FUNCTION
The effect of dust attenuation
Comparison with observations
CONCLUSIONS
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