The MOSDEF survey: the mass–metallicity relationship and the existence of the FMR at z ∼ 1.5

Author:

Topping Michael W12,Shapley Alice E1,Sanders Ryan L3ORCID,Kriek Mariska4,Reddy Naveen A5,Coil Alison L6,Mobasher Bahram5,Siana Brian5,Freeman William R5,Shivaei Irene2,Azadi Mojegan7,Price Sedona H8,Leung Gene C K6,Fetherolf Tara5,de Groot Laura9,Zick Tom4,Fornasini Francesca M7ORCID,Barro Guillermo10,Runco Jordan N1ORCID

Affiliation:

1. Department of Physics & Astronomy, University of California: Los Angeles, 430 Portola Plaza, Los Angeles, CA 90095, USA

2. Department of Astronomy / Steward Observatory, University of Arizona, 933 N Cherry Ave, Tucson, AZ 85721, USA

3. Department of Physics, University of California, Davis, One Shields Ave, Davis, CA 95616, USA

4. Department of Astronomy, University of California, Berkeley, CA 94720, USA

5. Department of Physics & Astronomy, University of California, Riverside, 900 University Avenue, Riverside, CA 92521, USA

6. Center for Astrophysics and Space Sciences, University of California, San Diego, 9500 Gilman Dr., La Jolla, CA 92093-0424, USA

7. Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138, USA

8. Max-Planck-Institut für Extraterrestrische Physik, Postfach 1312, Garching D-85741, Germany

9. Department of Physics, The College of Wooster, 1189 Beall Avenue, Wooster, OH 44691, USA

10. Department of Phyics, University of the Pacific, 3601 Pacific Ave, Stockton, CA 95211, USA

Abstract

ABSTRACT We analyse the rest-optical emission-line ratios of z ∼ 1.5 galaxies drawn from the Multi-Object Spectrometer for Infra-Red Exploration Deep Evolution Field (MOSDEF) survey. Using composite spectra, we investigate the mass–metallicity relation (MZR) at z ∼ 1.5 and measure its evolution to z = 0. When using gas-phase metallicities based on the N2 line ratio, we find that the MZR evolution from z ∼ 1.5 to z = 0 depends on stellar mass, evolving by $\Delta \rm log(\rm O/H) \sim 0.25$ dex at M*< $10^{9.75}\, \mathrm{M}_{\odot }$ down to $\Delta \rm log(\rm O/H) \sim 0.05$ at M* ≳ $10^{10.5}\, \mathrm{M}_{\odot }$. In contrast, the O3N2-based MZR shows a constant offset of $\Delta \rm log(\rm O/H) \sim 0.30$ across all masses, consistent with previous MOSDEF results based on independent metallicity indicators, and suggesting that O3N2 provides a more robust metallicity calibration for our z ∼ 1.5 sample. We investigated the secondary dependence of the MZR on star formation rate (SFR) by measuring correlated scatter about the mean M*-specific SFR and M*−$\log (\rm O3N2)$ relations. We find an anticorrelation between $\log (\rm O/H)$ and sSFR offsets, indicating the presence of a M*−SFR−Z relation, though with limited significance. Additionally, we find that our z ∼ 1.5 stacks lie along the z = 0 metallicity sequence at fixed μ = log (M*/M⊙) − 0.6 × $\log (\rm SFR / M_{\odot } \, yr^{-1})$ suggesting that the z ∼ 1.5 stacks can be described by the z = 0 fundamental metallicity relation (FMR). However, using different calibrations can shift the calculated metallicities off of the local FMR, indicating that appropriate calibrations are essential for understanding metallicity evolution with redshift. Finally, understanding how [N ii]/H α scales with galaxy properties is crucial to accurately describe the effects of blended [N ii] and H α on redshift and H α fiux measurements in future large surveys utilizing low-resolution spectra such as with Euclid and the Roman Space Telescope.

Funder

NSF

Space Telescope Science Institute

NASA

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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