Authors

A. Grazian, INAF–Osservatorio Astronomico di Roma, Italy
A. Fontana, INAF–Osservatorio Astronomico di Roma, Italy
P. Santini, INAF–Osservatorio Astronomico di Roma, Italy
J. S. Dunlop, University of Edinburgh, UK
H. C. Ferguson, Space Telescope Science Institute
M. Castellano, INAF–Osservatorio Astronomico di Roma, Italy
R. Amorin, INAF–Osservatorio Astronomico di Roma, Italy
M. L. N. Ashby, Harvard-Smithsonian Center for Astrophysics
G. Barro, University of California - Santa Cruz
P. Behroozi, Space Telescope Science Institute
K. Boutsia, INAF–Osservatorio Astronomico di Roma, Italy
K. I. Caputi, University of Groningen, the Netherlands
R. R. Chary, California Institute of Technology
A. Dekel, Hebrew University, Israel
M. E. Dickenson, NOAO
S. M. Faber, University of California - Santa Cruz
G. G. Fazio, Harvard-Smithsonian Center for Astrophysics
S. L. Finkelstein, University of Texas - Austin
A. Galametz, Max Planck Institute for Extraterrestrial Physics, Germany
E. Giallongo, INAF–Osservatorio Astronomico di Roma, Italy
M. Giavalisco, University of Massachusetts - Amherst
N. A. Grogin, Space Telescope Science Institute
Y. Guo, University of California - Santa Cruz
Dale D. Kocevski, University of KentuckyFollow
A. M. Koekemoer, Space Telescope Science Institute
D. C. Koo, University of California - Santa Cruz
K.-S. Lee, Purdue University
Y. Lu, Stanford University
E. Merlin, INAF–Osservatorio Astronomico di Roma, Italy
B. Mobasher, University of California - Riverside
M. Nonino, INAF–Osservatorio Astronomico di Trieste, Italy
C. Paovich, Texas A & M University
D. Paris, INAF–Osservatorio Astronomico di Roma, Italy
L. Pentericci, INAF–Osservatorio Astronomico di Roma, Italy
N. Reddy, University of California - Riverside
A. Renzini, INAF–Osservatorio Astronomico di Padova, Italy
B. Salmon, Texas A & M University
M. Salvato, Max Planck Institute for Extraterrestrial Physics, Germany
V. Sommariva, University of Bologna, Italy
M. Song, University of Texas - Austin
E. Vanzella, INAF–Osservatorio Astronomico di Bologna, Italy

Abstract

Context. The form and evolution of the galaxy stellar mass function (GSMF) at high redshifts provide crucial information on star formation history and mass assembly in the young Universe, close or even prior to the epoch of reionization.

Aims. We used the unique combination of deep optical/near-infrared/mid-infrared imaging provided by HST, Spitzer, and the VLT in the CANDELS-UDS, GOODS-South, and HUDF fields to determine the GSMF over the redshift range 3.5 ≤ z ≤ 7.5.

Methods. We used the HST WFC3/IR near-infrared imaging from CANDELS and HUDF09, reaching H ≃ 27 − 28.5 over a total area of 369 arcmin2, in combination with associated deep HST ACS optical data, deep Spitzer IRAC imaging from the SEDS programme, and deep Y and K-band VLT Hawk-I images from the HUGS programme, to select a galaxy sample with high-quality photometric redshifts. These have been calibrated with more than 150 spectroscopic redshifts in the range 3.5 ≤ z ≤ 7.5, resulting in an overall precision of σz/ (1 + z) ~ 0.037. With this database we have determined the low-mass end of the high-redshift GSMF with unprecedented precision, reaching down to masses as low as M ~ 109 M at z = 4 and ~6 × 109 M at z = 7.

Results. We find that the GSMF at 3.5 ≤ z ≤ 7.5 depends only slightly on the recipes adopted to measure the stellar masses, namely the photometric redshifts, the star formation histories, the nebular contribution, or the presence of AGN in the parent sample. The low-mass end of the GSMF is steeper than has been found at lower redshifts, but appears to be unchanged over the redshift range probed here. Meanwhile the high-mass end of the GSMF appears to evolve primarily in density, although there is also some evidence of evolution in characteristic mass. Our results are very different from previous mass function estimates based on converting UV galaxy luminosity functions into mass functions via tight mass-to-light relations. Integrating our evolving GSMF over mass, we find that the growth of stellar mass density is barely consistent with the time-integral of the star formation rate density over cosmic time at z> 4.

Conclusions. These results confirm the unique synergy of the CANDELS+HUDF, HUGS, and SEDS surveys for the discovery and study of moderate/low-mass galaxies at high redshifts, and reaffirm the importance of space-based infrared selection for the unbiased measurement of the evolving GSMF in the young Universe.

Document Type

Article

Publication Date

3-2015

Notes/Citation Information

Published in Astronomy & Astrophysics, v. 575, article A96, p. 1-25.

© ESO, 2015

The copyright holders have granted the permission for posting the article here.

Digital Object Identifier (DOI)

http://dx.doi.org/10.1051/0004-6361/201424750

Funding Information

We acknowledge financial contribution from the agreement ASI-INAF I/009/10/0. This work is based on observations taken by the CANDELS Multi-Cycle Treasury Program with the NASA/ESA HST, which is operated by the Association of Universities for Research in Astronomy, Inc., under NASA contract NAS5-26555. Observations were also carried out using the Very Large Telescope at the ESO Paranal Observatory under Programme IDs LP186.A-0898, LP181.A-0717, LP168.A-0485, ID 170.A-0788, ID 181.A-0485, ID 283.A-5052 and the ESO Science Archive under Programme IDs 60.A-9284, 67.A-0249, 71.A-0584, 73.A-0564, 68.A-0563, 69.A-0539, 70.A-0048, 64.O-0643, 66.A-0572, 68.A-0544, 164.O-0561, 163.N-0210, 85.A-0961 and 60.A-9120. This work is based in part on observations made with the Spitzer Space Telescope, which is operated by the Jet Propulsion Laboratory, California Institute of Technology under a contract with NASA. Support for this work was provided by NASA through an award issued by JPL/Caltech. A.F. and J.S.D. acknowledge the contribution of the EC FP7 SPACE project ASTRODEEP (Ref. No: 312725). J.S.D. also acknowledges the support of the Royal Society via a Wolfson Research Merit Award, and the support of the ERC through an Advanced Grant.

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