2016ApJ...825....5S


Query : 2016ApJ...825....5S

2016ApJ...825....5S - Astrophys. J., 825, 5-5 (2016/July-1)

The evolution of the galaxy stellar mass function at z = 4-8: a steepening low-mass-end slope with increasing redshift.

SONG M., FINKELSTEIN S.L., ASHBY M.L.N., GRAZIAN A., LU Y., PAPOVICH C., SALMON B., SOMERVILLE R.S., DICKINSON M., DUNCAN K., FABER S.M., FAZIO G.G., FERGUSON H.C., FONTANA A., GUO Y., HATHI N., LEE S.-K., MERLIN E. and WILLNER S.P.

Abstract (from CDS):

We present galaxy stellar mass functions (GSMFs) at z=4-8 from a rest-frame ultraviolet (UV) selected sample of ∼4500 galaxies, found via photometric redshifts over an area of ∼280 arcmin2 in the Cosmic Assembly Near-infrared Deep Extragalactic Legacy Survey (CANDELS)/Great Observatories Origins Deep Survey (GOODS) fields and the Hubble Ultra Deep Field. The deepest Spitzer/IRAC data 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 ( {M}_{UV} ) and logarithmic stellar mass ( log{M}_{* } ) that holds for galaxies with log({M}_{* }/{M}_☉)\lesssim 10 . We use simulations to validate our method of measuring the slope of the log{M}_{* } -MUV 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=4-8, while the normalization of the trend exhibits a weak evolution toward lower masses at higher redshift. We combine the log{M}_{* } -MUV 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}^{+0.08} at z=4 to α=-{2.25}_{-0.35}^{+0.72} at z=8. The inferred stellar mass density, when integrated over {M}_{* }={10}^{8} -1013 M☉, increases by a factor of {10}_{-2}^{+30} between z=7 and z=4 and is in good agreement with the time integral of the cosmic star formation rate density.

Abstract Copyright: © 2016. The American Astronomical Society. All rights reserved.

Journal keyword(s): galaxies: evolution - galaxies: formation - galaxies: high-redshift - galaxies: luminosity function, mass function

Simbad objects: 5

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Number of rows : 5
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 ACO 2744 ClG 00 14 20.03 -30 23 17.8           ~ 1077 0
2 NAME GOODS Southern Field reg 03 32 28.0 -27 48 30           ~ 1623 1
3 NAME Hubble Ultra Deep Field reg 03 32 39.0 -27 47 29           ~ 1900 0
4 MCS J0416.1-2403 ClG 04 16 08.380 -24 04 20.80           ~ 425 0
5 NAME GOODS-N Field reg 12 36 55.0 +62 14 15           ~ 1364 1

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