Abstract

ABSTRACT We present a new determination of the galaxy stellar-mass function (GSMF) over the redshift interval 0.25 ≤ z ≤ 3.75, derived from a combination of ground-based and Hubble Space Telescope (HST) imaging surveys. Based on a near-IR-selected galaxy sample selected over a raw survey area of 3 deg2 and spanning ≥4 dex in stellar mass, we fit the GSMF with both single and double Schechter functions, carefully accounting for Eddington bias to derive both observed and intrinsic parameter values. We find that a double Schechter function is a better fit to the GSMF at all redshifts, although the single and double Schechter function fits are statistically indistinguishable by z = 3.25. We find no evidence for significant evolution in M⋆, with the intrinsic value consistent with $\log _{10}(M^{\star }/\hbox{$\rm \, M_{\odot }$})=10.55\pm {0.1}$ over the full redshift range. Overall, our determination of the GSMF is in good agreement with recent simulation results, although differences persist at the highest stellar masses. Splitting our sample according to location on the UVJ plane, we find that the star-forming GSMF can be adequately described by a single Schechter function over the full redshift range, and has not evolved significantly since z ≃ 2.5. In contrast, both the normalization and the functional form of the passive GSMF evolve dramatically with redshift, switching from a single to a double Schechter function at z ≤ 1.5. As a result, we find that while passive galaxies dominate the integrated stellar-mass density at z ≤ 0.75, they only contribute ≲10 per cent by z ≃ 3. Finally, we provide a simple parametrization that provides an accurate estimate of the GSMF, both observed and intrinsic, at any redshift within the range 0 ≤ z ≤ 4.

Highlights

  • An accurate determination of the evolving galaxy stellar-mass function (GSMF) is crucial for improving our understanding of galaxy evolution

  • Given that the stellar-mass densities predicted by integrating the Madau & Dickinson (2014) fit to the cosmic star-formation rate density include the contribution from stellar remnants, it is clearly of interest to compare them to our direct results

  • In this paper we have presented a new derivation of the GSMF over the redshift interval 0.25 ≤ z ≤ 3.75, based on a near-IR selected galaxy sample covering a raw survey area of 3 deg2 and spanning ≥ 4 dex in stellar mass

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Summary

INTRODUCTION

An accurate determination of the evolving galaxy stellar-mass function (GSMF) is crucial for improving our understanding of galaxy evolution. At higher redshifts, studies arrive at different conclusions regarding the shape and evolution of the total GSMF and, in particular, the detectability, or otherwise, of an environmentally induced upturn in the number densities of low-mass passive galaxies at z ≥ 1 (e.g. Tomczak et al 2014; Davidzon et al 2017; Wright et al 2018) Within this context, the primary motivation for this study is to use a combination of the best available ground and space-based photometry, covering a sufficiently large cosmological volume and dynamic range in stellar mass, to accurately determine both the high and low-mass shape of the GSMF out to z 4.

Imaging data
The UKIDSS Ultra Deep Survey
UltraVISTA
CFHTLS-D1
CANDELS catalogues
CATALOGUE PRODUCTION AND SAMPLE SELECTION
Photometry catalogues
Photometric redshifts
Sample construction
Stellar masses
GSMF DETERMINATION
Number densities
Individual ground-based GSMF determinations
The combined HST and ground-based GSMF
Fitting the observed GSMF
Eddington bias
The intrinsic GSMF
Comparison to simulations
An evolving fit to the galaxy stellar mass function
THE PASSIVE AND STAR-FORMING GALAXY STELLAR MASS FUNCTIONS
UVJ selection
Schechter function fits
The star-forming GSMF
The passive GSMF
A comparison with the Peng et al model
THE INTEGRATED STELLAR-MASS DENSITY
Findings
CONCLUSIONS
Full Text
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