Monthly Notices of the Royal Astronomical Society · 2022 · 96 citations · 198 references
Natural SciencesAstronomyPhysicsAstrophysicsCosmologyStar FormationCosmic Star Formation HistoryGalaxy FormationMassive StarsObservational CosmologyRedshift SurveysCosmological SimulationsEmission-line Galaxy SurveysHigh-redshift GalaxiesHigh-redshift Star FormationSpecific Star Formation RateStar Formation Rates In GalaxiesStar Formation SimulationsStar-forming Galaxies
Abstract We introduce SERRA, a suite of zoom-in high-resolution (1.2 × 104 M⊙, ≃ 25 pc at z = 7.7) cosmological simulations including non-equilibrium chemistry and on-the-fly radiative transfer. The outputs are post-processed to derive galaxy UV+FIR continuum and emission line properties. Results are compared with available multi-wavelength data to constrain the physical properties (e.g. star formation rates, stellar/gas/dust mass, metallicity) of high-redshift 6 ≲ z ≲ 15 galaxies. This flagship paper focuses on the z = 7.7 sub-sample, including 202 galaxies with stellar mass 107 M⊙ ≲ M⋆ ≲ 5 × 1010 M⊙, and specific star formation ranging from sSFR ∼ 100 Gyr−1 in young, low-mass galaxies to ∼10 Gyr−1 for older, massive ones. At this redshift, serra galaxies are typically bursty, i.e. they are located above the Schmidt-Kennicutt relation by a factor $\kappa _s = 3.03^{+4.9}_{-1.8}$, consistent with recent findings for [O iii] and [C ii] emitters at high-z. They also show relatively large IRX =LFIR/LUV values as a result of their compact/clumpy morphology effectively blocking the stellar UV luminosity. Note that this conclusion might be affected by insufficient spatial resolution at the molecular cloud level. We confirm that early galaxies lie on the standard [C ii]$-\rm SFR$ relation; their observed L[OIII]/L[CII] ≃ 1 − 10 ratios can be reproduced by a part of the SERRA galaxies without the need of a top-heavy IMF and/or anomalous C/O abundances. [O i] line intensities are similar to local ones, making ALMA high-z detections challenging but feasible ($\sim 6\, \rm hr$ for an SFR of 50 M⊙ yr−1).
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