The Direct-method Oxygen Abundance of Typical Dwarf Galaxies at Cosmic High Noon

We present a Keck/MOSFIRE rest-optical composite spectrum of 16 typical gravitationally lensed star-forming dwarf galaxies at 1.7 ≲ z ≲ 2.6 ( z _mean = 2.30), all chosen independent of emission-line strength. These galaxies have a median stellar mass of $\mathrm{log}{({M}_{* }/{M}_{\odot })}_{\mathr...

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Main Authors: Timothy Gburek, Brian Siana, Anahita Alavi, Najmeh Emami, Johan Richard, William R. Freeman, Daniel P. Stark, Christopher Snapp-Kolas
Format: Article
Language:English
Published: IOP Publishing 2023-01-01
Series:The Astrophysical Journal
Subjects:
Online Access:https://doi.org/10.3847/1538-4357/acb153
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author Timothy Gburek
Brian Siana
Anahita Alavi
Najmeh Emami
Johan Richard
William R. Freeman
Daniel P. Stark
Christopher Snapp-Kolas
author_facet Timothy Gburek
Brian Siana
Anahita Alavi
Najmeh Emami
Johan Richard
William R. Freeman
Daniel P. Stark
Christopher Snapp-Kolas
author_sort Timothy Gburek
collection DOAJ
description We present a Keck/MOSFIRE rest-optical composite spectrum of 16 typical gravitationally lensed star-forming dwarf galaxies at 1.7 ≲ z ≲ 2.6 ( z _mean = 2.30), all chosen independent of emission-line strength. These galaxies have a median stellar mass of $\mathrm{log}{({M}_{* }/{M}_{\odot })}_{\mathrm{med}}={8.29}_{-0.43}^{+0.51}$ and a median star formation rate of ${{\rm{S}}{\rm{F}}{\rm{R}}}_{{\rm{H}}\alpha }^{{\rm{m}}{\rm{e}}{\rm{d}}}={2.25}_{-1.26}^{+2.15}\,{M}_{\odot }\,{{\rm{y}}{\rm{r}}}^{-1}$ . We measure the faint electron-temperature-sensitive [O iii ] λ 4363 emission line at 2.5 σ (4.1 σ ) significance when considering a bootstrapped (statistical-only) uncertainty spectrum. This yields a direct-method oxygen abundance of $12+\mathrm{log}{({\rm{O}}/{\rm{H}})}_{\mathrm{direct}}={7.88}_{-0.22}^{+0.25}$ ( ${0.15}_{-0.06}^{+0.12}\ {Z}_{\odot }$ ). We investigate the applicability at high z of locally calibrated oxygen-based strong-line metallicity relations, finding that the local reference calibrations of Bian et al. best reproduce (≲0.12 dex) our composite metallicity at fixed strong-line ratio. At fixed M _* , our composite is well represented by the z ∼ 2.3 direct-method stellar mass—gas-phase metallicity relation (MZR) of Sanders et al. When comparing to predicted MZRs from the IllustrisTNG and FIRE simulations, having recalculated our stellar masses with more realistic nonparametric star formation histories $(\mathrm{log}{({M}_{* }/{M}_{\odot })}_{\mathrm{med}}={8.92}_{-0.22}^{+0.31})$ , we find excellent agreement with the FIRE MZR. Our composite is consistent with no metallicity evolution, at fixed M _* and SFR, of the locally defined fundamental metallicity relation. We measure the doublet ratio [O ii ] λ 3729/[O ii ] λ 3726 = 1.56 ± 0.32 (1.51 ± 0.12) and a corresponding electron density of ${n}_{e}={1}_{-0}^{+215}\ {\mathrm{cm}}^{-3}$ ( ${n}_{e}={1}_{-0}^{+74}\ {\mathrm{cm}}^{-3}$ ) when considering the bootstrapped (statistical-only) error spectrum. This result suggests that lower-mass galaxies have lower densities than higher-mass galaxies at z ∼ 2.
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spelling doaj.art-30b8dfa48ed34e3daf295897b05e60852023-09-03T13:42:31ZengIOP PublishingThe Astrophysical Journal1538-43572023-01-01948210810.3847/1538-4357/acb153The Direct-method Oxygen Abundance of Typical Dwarf Galaxies at Cosmic High NoonTimothy Gburek0https://orcid.org/0000-0002-7732-9205Brian Siana1https://orcid.org/0000-0002-4935-9511Anahita Alavi2https://orcid.org/0000-0002-8630-6435Najmeh Emami3https://orcid.org/0000-0003-2047-1689Johan Richard4https://orcid.org/0000-0001-5492-1049William R. Freeman5https://orcid.org/0000-0003-3559-5270Daniel P. Stark6Christopher Snapp-Kolas7https://orcid.org/0000-0002-9593-0053Department of Physics & Astronomy, University of California , Riverside, CA 92521, USA ; timothy.gburek@email.ucr.eduDepartment of Physics & Astronomy, University of California , Riverside, CA 92521, USA ; timothy.gburek@email.ucr.eduIPAC, California Institute of Technology , 1200 E. California Boulevard, Pasadena, CA 91125, USAMinnesota Institute for Astrophysics, University of Minnesota , Minneapolis, MN, 55455, USAUniv Lyon , Univ Lyon1, Ens de Lyon, CNRS, Centre de Recherche Astrophysique de Lyon UMR5574, F-69230, Saint-Genis-Laval, FranceDepartment of Physics & Astronomy, University of California , Riverside, CA 92521, USA ; timothy.gburek@email.ucr.eduSteward Observatory, University of Arizona , 933 N. Cherry Ave, Tucson, AZ 85721, USADepartment of Physics & Astronomy, University of California , Riverside, CA 92521, USA ; timothy.gburek@email.ucr.eduWe present a Keck/MOSFIRE rest-optical composite spectrum of 16 typical gravitationally lensed star-forming dwarf galaxies at 1.7 ≲ z ≲ 2.6 ( z _mean = 2.30), all chosen independent of emission-line strength. These galaxies have a median stellar mass of $\mathrm{log}{({M}_{* }/{M}_{\odot })}_{\mathrm{med}}={8.29}_{-0.43}^{+0.51}$ and a median star formation rate of ${{\rm{S}}{\rm{F}}{\rm{R}}}_{{\rm{H}}\alpha }^{{\rm{m}}{\rm{e}}{\rm{d}}}={2.25}_{-1.26}^{+2.15}\,{M}_{\odot }\,{{\rm{y}}{\rm{r}}}^{-1}$ . We measure the faint electron-temperature-sensitive [O iii ] λ 4363 emission line at 2.5 σ (4.1 σ ) significance when considering a bootstrapped (statistical-only) uncertainty spectrum. This yields a direct-method oxygen abundance of $12+\mathrm{log}{({\rm{O}}/{\rm{H}})}_{\mathrm{direct}}={7.88}_{-0.22}^{+0.25}$ ( ${0.15}_{-0.06}^{+0.12}\ {Z}_{\odot }$ ). We investigate the applicability at high z of locally calibrated oxygen-based strong-line metallicity relations, finding that the local reference calibrations of Bian et al. best reproduce (≲0.12 dex) our composite metallicity at fixed strong-line ratio. At fixed M _* , our composite is well represented by the z ∼ 2.3 direct-method stellar mass—gas-phase metallicity relation (MZR) of Sanders et al. When comparing to predicted MZRs from the IllustrisTNG and FIRE simulations, having recalculated our stellar masses with more realistic nonparametric star formation histories $(\mathrm{log}{({M}_{* }/{M}_{\odot })}_{\mathrm{med}}={8.92}_{-0.22}^{+0.31})$ , we find excellent agreement with the FIRE MZR. Our composite is consistent with no metallicity evolution, at fixed M _* and SFR, of the locally defined fundamental metallicity relation. We measure the doublet ratio [O ii ] λ 3729/[O ii ] λ 3726 = 1.56 ± 0.32 (1.51 ± 0.12) and a corresponding electron density of ${n}_{e}={1}_{-0}^{+215}\ {\mathrm{cm}}^{-3}$ ( ${n}_{e}={1}_{-0}^{+74}\ {\mathrm{cm}}^{-3}$ ) when considering the bootstrapped (statistical-only) error spectrum. This result suggests that lower-mass galaxies have lower densities than higher-mass galaxies at z ∼ 2.https://doi.org/10.3847/1538-4357/acb153Galaxy abundancesDwarf galaxiesHigh-redshift galaxiesGalaxy evolutionInterstellar mediumScaling relations
spellingShingle Timothy Gburek
Brian Siana
Anahita Alavi
Najmeh Emami
Johan Richard
William R. Freeman
Daniel P. Stark
Christopher Snapp-Kolas
The Direct-method Oxygen Abundance of Typical Dwarf Galaxies at Cosmic High Noon
The Astrophysical Journal
Galaxy abundances
Dwarf galaxies
High-redshift galaxies
Galaxy evolution
Interstellar medium
Scaling relations
title The Direct-method Oxygen Abundance of Typical Dwarf Galaxies at Cosmic High Noon
title_full The Direct-method Oxygen Abundance of Typical Dwarf Galaxies at Cosmic High Noon
title_fullStr The Direct-method Oxygen Abundance of Typical Dwarf Galaxies at Cosmic High Noon
title_full_unstemmed The Direct-method Oxygen Abundance of Typical Dwarf Galaxies at Cosmic High Noon
title_short The Direct-method Oxygen Abundance of Typical Dwarf Galaxies at Cosmic High Noon
title_sort direct method oxygen abundance of typical dwarf galaxies at cosmic high noon
topic Galaxy abundances
Dwarf galaxies
High-redshift galaxies
Galaxy evolution
Interstellar medium
Scaling relations
url https://doi.org/10.3847/1538-4357/acb153
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