The AURORA Survey: The Mass -- Metallicity and Fundamental Metallicity Relations at $z \sim 2.3$ Based Purely on Direct $T_e$ Metallicities
Ali Ahmad Khostovan, Ryan L. Sanders, Alice E. Shapley, Michael W. Topping, Naveen A. Reddy, Alex M. Garcia, Danielle A. Berg, Leonardo Clarke, Fergus Cullen, Richard S. Ellis, N. M. Förster Schreiber, Karl Glazebrook, Tucker Jones, Derek J. McLeod, Anthony J. Pahl, Max Pettini, Paul Torrey
TL;DR
This work delivers direct $T_e$-based constraints on the Mass--Metallicity Relation (MZR) and Fundamental Metallicity Relation (FMR) at cosmic noon ($z\sim2.3$) using 34 galaxies from the AURORA JWST/NIRSpec survey, including dual-zone $T_e$ measurements from [O III]4363 and [O II]7320,7331. The authors derive precise stellar masses and SFRs via SED fitting with nebular emission and a metallicity-dependent SFR calibration, revealing a MZR with slope $\gamma=0.27\pm0.04$, normalization $12+\log(O/H)=8.44\pm0.04$ at $M_\star=10^{10}\,M_\odot$, and intrinsic scatter $0.10\pm0.02$ dex; the $z\sim2$ FMR is consistent with $z\sim0$ calibrations within $\sim0.1$ dex. Comparisons to six simulations show none reproduce the observed $z\sim2$ MZR normalization evolution, highlighting gaps in chemical-enrichment and feedback modeling at cosmic noon, though selection effects may bias low-Hydrogen measurements toward higher SFR. The results imply smooth secular chemical evolution already in place by $z\sim2$ and demonstrate JWST’s power to anchor simulations with direct metallicity measurements across a broad parameter space, paving the way for larger, less-biased samples.
Abstract
We present new constraints on the Mass -- Metallicity (MZR) and Fundamental Metallicity Relations (FMR) using a sample of 34 galaxies at $1.38\leq~z\leq~3.5$ (median $z=2.28$). These galaxies have direct $T_e$ measurements from [O\sc{iii}]4363Å~and/or [O\sc{ii}]7320,7331Å~auroral emission lines detected with \textit{JWST}/NIRSpec as part of the AURORA survey. The detection of both oxygen auroral lines allows for dual-zone direct $T_e$ measurements and expands the dynamic range in $12+\log\mathrm{(O/H)}$ (7.68 to 8.65 dex), stellar mass ($10^{8}$ to $10^{10.4}$ M$_\odot$), and star-formation rate ($1$ to $100$ M$_\odot$ yr$^{-1}$) compared to previous direct $T_e$ studies of the high-redshift MZR and FMR. We characterize the $z\sim2$ MZR and find a slope of $0.27\pm0.04$ and normalization of $12+\log\mathrm{(O/H)} = 8.44\pm0.04$ at $10^{10}$ M$_\odot$ with an intrinsic scatter of 0.10 dex, consistent with past strong-line MZR measurements. Comparisons with $z\sim2$ predictions from six simulations reveal that none reproduce our observed MZR normalization evolution between $z\sim0$ and $z\sim2$. This discrepancy suggests current models do not fully capture the chemical enrichment and feedback processes occurring at cosmic noon. However, all 34 galaxies are on or above the star-forming main sequence such that our sample may be biased towards lower $12+\log\mathrm{(O/H)}$ if the FMR persists at $z\sim2$. Correcting for this selection effect would increase O/H by $\approx0.1$ dex at 10$^{9.3}$ M$_\odot$ (the median mass of our sample) bringing our MZR into better agreement with that of \texttt{TNG}. Lastly, we find our $z\sim2.3$ sample is consistent with the $z\sim0$ FMR within 0.1 dex in O/H, indicating that the smooth secular mechanisms regulating chemical enrichment, star formation, stellar mass, and outflows were in place at cosmic noon.
