A deep radio view of the evolution of the cosmic star formation rate density from a stellar-mass-selected sample in VLA-COSMOS

We present the 1.4 GHz radio luminosity functions (RLFs) of galaxies in the Cosmic Evolution Survey (COSMOS) field, measured above and below the 5σ detection threshold, using a Bayesian model-fitting technique. The radio flux densities from Very Large Array (VLA)-COSMOS 3-GHz data are extr...

Full description

Bibliographic Details
Main Authors: Malefahlo, ED, Jarvis, MJ, Santos, MG, White, SV, Adams, NJ, Bowler, RAA
Format: Journal article
Language:English
Published: Oxford University Press 2021
_version_ 1797107598384693248
author Malefahlo, ED
Jarvis, MJ
Santos, MG
White, SV
Adams, NJ
Bowler, RAA
author_facet Malefahlo, ED
Jarvis, MJ
Santos, MG
White, SV
Adams, NJ
Bowler, RAA
author_sort Malefahlo, ED
collection OXFORD
description We present the 1.4 GHz radio luminosity functions (RLFs) of galaxies in the Cosmic Evolution Survey (COSMOS) field, measured above and below the 5σ detection threshold, using a Bayesian model-fitting technique. The radio flux densities from Very Large Array (VLA)-COSMOS 3-GHz data are extracted at the position of stellar-mass-selected galaxies. We fit a local RLF model, which is a combination of active galactic nuclei and star-forming galaxies (SFGs), in 10 redshift bins with a pure luminosity evolution model. Our RLF exceeds previous determinations at low radio luminosities at z < 1.6 with the same radio data, due to our ability to directly constrain the knee and faint-end slope of the RLF. Beyond z ∼2, we find that the SFG part of the RLF exhibits a negative evolution (L∗ moves to lower luminosities) due to the decrease in low stellar-mass galaxies in our sample at high redshifts. From the RLF for SFGs, we determine the evolution in the cosmic star formation rate density (SFRD), which we find to be consistent with the established behaviour up to z ∼1 using far-infrared data, but exceeds that from the previous radio-based work for the reasons highlighted above. Beyond z ∼1.5 the cosmic SFRD declines. We note that the relation between radio luminosity and star formation rate is crucial in measuring the cosmic SFRD from radio data at z > 1.5. We investigate the effects of stellar mass on the total RLF by splitting our sample into low (108.5 ≤ M/M ≤ 1010) and high ($Mgt 10^{10}, mathrm{M}_{odot }$) stellar-mass subsets. We find that the SFRD is dominated by sources in the high stellar masses bin, at all redshifts.
first_indexed 2024-03-07T07:18:16Z
format Journal article
id oxford-uuid:57538581-ed99-4ddf-b883-3a599b93f218
institution University of Oxford
language English
last_indexed 2024-03-07T07:18:16Z
publishDate 2021
publisher Oxford University Press
record_format dspace
spelling oxford-uuid:57538581-ed99-4ddf-b883-3a599b93f2182022-09-07T06:55:52ZA deep radio view of the evolution of the cosmic star formation rate density from a stellar-mass-selected sample in VLA-COSMOSJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:57538581-ed99-4ddf-b883-3a599b93f218EnglishSymplectic ElementsOxford University Press2021Malefahlo, EDJarvis, MJSantos, MGWhite, SVAdams, NJBowler, RAAWe present the 1.4 GHz radio luminosity functions (RLFs) of galaxies in the Cosmic Evolution Survey (COSMOS) field, measured above and below the 5σ detection threshold, using a Bayesian model-fitting technique. The radio flux densities from Very Large Array (VLA)-COSMOS 3-GHz data are extracted at the position of stellar-mass-selected galaxies. We fit a local RLF model, which is a combination of active galactic nuclei and star-forming galaxies (SFGs), in 10 redshift bins with a pure luminosity evolution model. Our RLF exceeds previous determinations at low radio luminosities at z < 1.6 with the same radio data, due to our ability to directly constrain the knee and faint-end slope of the RLF. Beyond z ∼2, we find that the SFG part of the RLF exhibits a negative evolution (L∗ moves to lower luminosities) due to the decrease in low stellar-mass galaxies in our sample at high redshifts. From the RLF for SFGs, we determine the evolution in the cosmic star formation rate density (SFRD), which we find to be consistent with the established behaviour up to z ∼1 using far-infrared data, but exceeds that from the previous radio-based work for the reasons highlighted above. Beyond z ∼1.5 the cosmic SFRD declines. We note that the relation between radio luminosity and star formation rate is crucial in measuring the cosmic SFRD from radio data at z > 1.5. We investigate the effects of stellar mass on the total RLF by splitting our sample into low (108.5 ≤ M/M ≤ 1010) and high ($Mgt 10^{10}, mathrm{M}_{odot }$) stellar-mass subsets. We find that the SFRD is dominated by sources in the high stellar masses bin, at all redshifts.
spellingShingle Malefahlo, ED
Jarvis, MJ
Santos, MG
White, SV
Adams, NJ
Bowler, RAA
A deep radio view of the evolution of the cosmic star formation rate density from a stellar-mass-selected sample in VLA-COSMOS
title A deep radio view of the evolution of the cosmic star formation rate density from a stellar-mass-selected sample in VLA-COSMOS
title_full A deep radio view of the evolution of the cosmic star formation rate density from a stellar-mass-selected sample in VLA-COSMOS
title_fullStr A deep radio view of the evolution of the cosmic star formation rate density from a stellar-mass-selected sample in VLA-COSMOS
title_full_unstemmed A deep radio view of the evolution of the cosmic star formation rate density from a stellar-mass-selected sample in VLA-COSMOS
title_short A deep radio view of the evolution of the cosmic star formation rate density from a stellar-mass-selected sample in VLA-COSMOS
title_sort deep radio view of the evolution of the cosmic star formation rate density from a stellar mass selected sample in vla cosmos
work_keys_str_mv AT malefahloed adeepradioviewoftheevolutionofthecosmicstarformationratedensityfromastellarmassselectedsampleinvlacosmos
AT jarvismj adeepradioviewoftheevolutionofthecosmicstarformationratedensityfromastellarmassselectedsampleinvlacosmos
AT santosmg adeepradioviewoftheevolutionofthecosmicstarformationratedensityfromastellarmassselectedsampleinvlacosmos
AT whitesv adeepradioviewoftheevolutionofthecosmicstarformationratedensityfromastellarmassselectedsampleinvlacosmos
AT adamsnj adeepradioviewoftheevolutionofthecosmicstarformationratedensityfromastellarmassselectedsampleinvlacosmos
AT bowlerraa adeepradioviewoftheevolutionofthecosmicstarformationratedensityfromastellarmassselectedsampleinvlacosmos
AT malefahloed deepradioviewoftheevolutionofthecosmicstarformationratedensityfromastellarmassselectedsampleinvlacosmos
AT jarvismj deepradioviewoftheevolutionofthecosmicstarformationratedensityfromastellarmassselectedsampleinvlacosmos
AT santosmg deepradioviewoftheevolutionofthecosmicstarformationratedensityfromastellarmassselectedsampleinvlacosmos
AT whitesv deepradioviewoftheevolutionofthecosmicstarformationratedensityfromastellarmassselectedsampleinvlacosmos
AT adamsnj deepradioviewoftheevolutionofthecosmicstarformationratedensityfromastellarmassselectedsampleinvlacosmos
AT bowlerraa deepradioviewoftheevolutionofthecosmicstarformationratedensityfromastellarmassselectedsampleinvlacosmos