The LOFAR two-metre sky survey deep fields: the star-formation rate–radio luminosity relation at low frequencies

In this paper, we investigate the relationship between 150 MHz luminosity and the star-formation rate – the SFR-L150 MHz relation – using 150 MHz measurements for a near-infrared selected sample of 118 517 z < 1 galaxies. New radio survey data offer compelling advantages over previous generation...

Полное описание

Библиографические подробности
Главные авторы: Smith, DJB, Haskell, P, Gürkan, G, Best, PN, Hardcastle, MJ, Kondapally, R, Williams, W, Duncan, KJ, Cochrane, RK, McCheyne, I, Röttgering, HJA, Sabater, J, Shimwell, TW, Tasse, C, Bonato, M, Bondi, M, Jarvis, MJ, Leslie, SK, Prandoni, I, Wang, L
Формат: Journal article
Язык:English
Опубликовано: EDP Sciences 2021
_version_ 1826295595296358400
author Smith, DJB
Haskell, P
Gürkan, G
Best, PN
Hardcastle, MJ
Kondapally, R
Williams, W
Duncan, KJ
Cochrane, RK
McCheyne, I
Röttgering, HJA
Sabater, J
Shimwell, TW
Tasse, C
Bonato, M
Bondi, M
Jarvis, MJ
Leslie, SK
Prandoni, I
Wang, L
author_facet Smith, DJB
Haskell, P
Gürkan, G
Best, PN
Hardcastle, MJ
Kondapally, R
Williams, W
Duncan, KJ
Cochrane, RK
McCheyne, I
Röttgering, HJA
Sabater, J
Shimwell, TW
Tasse, C
Bonato, M
Bondi, M
Jarvis, MJ
Leslie, SK
Prandoni, I
Wang, L
author_sort Smith, DJB
collection OXFORD
description In this paper, we investigate the relationship between 150 MHz luminosity and the star-formation rate – the SFR-L150 MHz relation – using 150 MHz measurements for a near-infrared selected sample of 118 517 z < 1 galaxies. New radio survey data offer compelling advantages over previous generation surveys for studying star formation in galaxies, including huge increases in sensitivity, survey speed, and resolution, while remaining impervious to extinction. The LOFAR Surveys Key Science Project is transforming our understanding of the low-frequency radio sky, with the 150 MHz data over the European Large Area Infrared Space Observatory Survey-North 1 field reaching an rms sensitivity of 20 μJy beam−1 over 10 deg2 at 6 arcsec resolution. All of the galaxies studied have SFR and stellar mass estimates that were derived from energy balance spectral energy distribution fitting using redshifts and aperture-matched forced photometry from the LOFAR Two-metre Sky Survey (LoTSS) Deep Fields data release. The impact of active galactic nuclei (AGN) is minimised by leveraging the deep ancillary data in the LoTSS data release, alongside median-likelihood methods that we demonstrate are resistant to AGN contamination. We find a linear and non-evolving SFR-L150 MHz relation, apparently consistent with expectations based on calorimetric arguments, down to the lowest SFRs < 0.01M⊙ yr−1. However, we also recover compelling evidence for stellar mass dependence in line with previous work on this topic, in the sense that higher mass galaxies have a larger 150 MHz luminosity at a given SFR, suggesting that the overall agreement with calorimetric arguments may be a coincidence. We conclude that, in the absence of AGN, 150 MHz observations can be used to measure accurate galaxy SFRs out to z = 1 at least, but it is necessary to account for stellar mass in the estimation in order to obtain 150 MHz-derived SFRs accurate to better than 0.5 dex. Our best-fit relation is log10(L150 MHz ∕W Hz−1) = (0.90 ± 0.01)log10(ψ∕M⊙ yr−1) + (0.33 ± 0.04)log10(M∕1010M⊙) + 22.22 ± 0.02.
first_indexed 2024-03-07T04:03:27Z
format Journal article
id oxford-uuid:c55e3014-9b57-4fb4-b1b6-219ad3fbebfb
institution University of Oxford
language English
last_indexed 2024-03-07T04:03:27Z
publishDate 2021
publisher EDP Sciences
record_format dspace
spelling oxford-uuid:c55e3014-9b57-4fb4-b1b6-219ad3fbebfb2022-03-27T06:30:18ZThe LOFAR two-metre sky survey deep fields: the star-formation rate–radio luminosity relation at low frequenciesJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:c55e3014-9b57-4fb4-b1b6-219ad3fbebfbEnglishSymplectic ElementsEDP Sciences2021Smith, DJBHaskell, PGürkan, GBest, PNHardcastle, MJKondapally, RWilliams, WDuncan, KJCochrane, RKMcCheyne, IRöttgering, HJASabater, JShimwell, TWTasse, CBonato, MBondi, MJarvis, MJLeslie, SKPrandoni, IWang, LIn this paper, we investigate the relationship between 150 MHz luminosity and the star-formation rate – the SFR-L150 MHz relation – using 150 MHz measurements for a near-infrared selected sample of 118 517 z < 1 galaxies. New radio survey data offer compelling advantages over previous generation surveys for studying star formation in galaxies, including huge increases in sensitivity, survey speed, and resolution, while remaining impervious to extinction. The LOFAR Surveys Key Science Project is transforming our understanding of the low-frequency radio sky, with the 150 MHz data over the European Large Area Infrared Space Observatory Survey-North 1 field reaching an rms sensitivity of 20 μJy beam−1 over 10 deg2 at 6 arcsec resolution. All of the galaxies studied have SFR and stellar mass estimates that were derived from energy balance spectral energy distribution fitting using redshifts and aperture-matched forced photometry from the LOFAR Two-metre Sky Survey (LoTSS) Deep Fields data release. The impact of active galactic nuclei (AGN) is minimised by leveraging the deep ancillary data in the LoTSS data release, alongside median-likelihood methods that we demonstrate are resistant to AGN contamination. We find a linear and non-evolving SFR-L150 MHz relation, apparently consistent with expectations based on calorimetric arguments, down to the lowest SFRs < 0.01M⊙ yr−1. However, we also recover compelling evidence for stellar mass dependence in line with previous work on this topic, in the sense that higher mass galaxies have a larger 150 MHz luminosity at a given SFR, suggesting that the overall agreement with calorimetric arguments may be a coincidence. We conclude that, in the absence of AGN, 150 MHz observations can be used to measure accurate galaxy SFRs out to z = 1 at least, but it is necessary to account for stellar mass in the estimation in order to obtain 150 MHz-derived SFRs accurate to better than 0.5 dex. Our best-fit relation is log10(L150 MHz ∕W Hz−1) = (0.90 ± 0.01)log10(ψ∕M⊙ yr−1) + (0.33 ± 0.04)log10(M∕1010M⊙) + 22.22 ± 0.02.
spellingShingle Smith, DJB
Haskell, P
Gürkan, G
Best, PN
Hardcastle, MJ
Kondapally, R
Williams, W
Duncan, KJ
Cochrane, RK
McCheyne, I
Röttgering, HJA
Sabater, J
Shimwell, TW
Tasse, C
Bonato, M
Bondi, M
Jarvis, MJ
Leslie, SK
Prandoni, I
Wang, L
The LOFAR two-metre sky survey deep fields: the star-formation rate–radio luminosity relation at low frequencies
title The LOFAR two-metre sky survey deep fields: the star-formation rate–radio luminosity relation at low frequencies
title_full The LOFAR two-metre sky survey deep fields: the star-formation rate–radio luminosity relation at low frequencies
title_fullStr The LOFAR two-metre sky survey deep fields: the star-formation rate–radio luminosity relation at low frequencies
title_full_unstemmed The LOFAR two-metre sky survey deep fields: the star-formation rate–radio luminosity relation at low frequencies
title_short The LOFAR two-metre sky survey deep fields: the star-formation rate–radio luminosity relation at low frequencies
title_sort lofar two metre sky survey deep fields the star formation rate radio luminosity relation at low frequencies
work_keys_str_mv AT smithdjb thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT haskellp thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT gurkang thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT bestpn thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT hardcastlemj thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT kondapallyr thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT williamsw thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT duncankj thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT cochranerk thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT mccheynei thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT rottgeringhja thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT sabaterj thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT shimwelltw thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT tassec thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT bonatom thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT bondim thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT jarvismj thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT lesliesk thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT prandonii thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT wangl thelofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT smithdjb lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT haskellp lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT gurkang lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT bestpn lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT hardcastlemj lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT kondapallyr lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT williamsw lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT duncankj lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT cochranerk lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT mccheynei lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT rottgeringhja lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT sabaterj lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT shimwelltw lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT tassec lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT bonatom lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT bondim lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT jarvismj lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT lesliesk lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT prandonii lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies
AT wangl lofartwometreskysurveydeepfieldsthestarformationrateradioluminosityrelationatlowfrequencies