Abstract

We present galaxy stellar mass functions (GSMFs) at z=z= 4-8 from a rest-frame ultraviolet (UV) selected sample of ∼\sim4500 galaxies, found via photometric redshifts over an area of ∼\sim280 arcmin2^2 in the CANDELS/GOODS fields and the Hubble Ultra Deep Field. The deepest Spitzer/IRAC data yet-to-date and the relatively large volume allow us to place a better constraint at both the low- and high-mass ends of the GSMFs compared to previous space-based studies from pre-CANDELS observations. Supplemented by a stacking analysis, we find a linear correlation between the rest-frame UV absolute magnitude at 1500 Å (MUVM_{\rm UV}) and logarithmic stellar mass (log⁡M∗\log M_*) that holds for galaxies with log⁡(M∗/M⊙)≲10\log(M_*/M_{\odot}) \lesssim 10. We use simulations to validate our method of measuring the slope of the log⁡M∗\log M_*-MUVM_{\rm UV} relation, finding that the bias is minimized with a hybrid technique combining photometry of individual bright galaxies with stacked photometry for faint galaxies. The resultant measured slopes do not significantly evolve over z=z= 4-8, while the normalization of the trend exhibits a weak evolution toward lower masses at higher redshift. We combine the log⁡M∗\log M_*-MUVM_{\rm UV} distribution with observed rest-frame UV luminosity functions at each redshift to derive the GSMFs, finding that the low-mass-end slope becomes steeper with increasing redshift from α=−1.55−0.07+0.08α=-1.55^{+0.08}_{-0.07} at z=4z=4 to α=−2.25−0.35+0.72α=-2.25^{+0.72}_{-0.35} at z=8z=8. The inferred stellar mass density, when integrated over M∗=108M_*=10^8-1013M⊙10^{13} M_{\odot}, increases by a factor of 10−2+3010^{+30}_{-2} between z=7z=7 and z=4z=4 and is in good agreement with the time integral of the cosmic star formation rate density.

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