Abstract

ABSTRACT We include a fully coupled treatment of metal and dust enrichment into the Delphi semi-analytic model of galaxy formation to explain the dust content of 13 Lyman break galaxies (LBGs) detected by the Atacama Large millimetre Array (ALMA) REBELS Large Program at z ≃ 7. We find that the galaxy dust mass, Md, is regulated by the combination of Type II supernova dust production, astration, shock destruction, and ejection in outflows; grain growth (with a standard time-scale τ0 = 30 Myr) plays a negligible role. The model predicts a dust-to-stellar mass ratio of $\sim 0.07\!-\!0.1{{\ \rm per\ cent}}$ and a UV-to-total star formation rate relation such that log(ψUV) = −0.05 [log(ψ)]2 + 0.86 log(ψ) − 0.05 (implying that 55–80 per cent of the star formation is obscured) for REBELS galaxies with stellar mass $M_* = 10^{9}\!-\!10^{10} \rm M_\odot$. This relation reconciles the intrinsic UV luminosity of LBGs with their observed luminosity function at z = 7. However, 2 out of the 13 systems show dust-to-stellar mass ratios ($\sim 0.94\!-\!1.1{{\ \rm per\ cent}}$) that are up to 18 times larger than expected from the fiducial relation. Due to the physical coupling between dust and metal enrichment, even decreasing τ0 to very low values (0.3 Myr) only increases the dust-to-stellar mass ratio by a factor of ∼2. Given that grain growth is not a viable explanation for such high observed ratios of the dust-to-stellar mass, we propose alternative solutions.

Highlights

  • Over the past decade instruments such as the Hubble Space Telescope (HST), Very large Telescope (VLT), Subaru and Keck have been used to assemble statistically large sample of high-redshift (z ∼> 5) Lyman break Galaxies (LBGs) at restframe ultra-violet (UV) wavelengths

  • A number of zoom-in simulations have been crucial in understanding the role of a range of interstellar medium (ISM) processes such as dust growth and dissociation, Supernova (SN) shock destruction, ISM dust grain growth and gas drag effects - on the dust distribution and its grain-size distribution in individual galaxies (Bekki 2015; Aoyama et al 2017; McKinnon et al 2018)

  • Similar in spirit to the semi-analytic models noted above (e.g. Popping et al 2017; Vijayan et al 2019; Triani et al 2020), the key strengths of this work lie in the fact that: (i) it uses a minimal number of mass- and redshift-independent free parameters to model the key physics of early galaxies; (ii) contrary to the other models which have been calibrated against low-redshift (z ∼ 0 − 3) data, our model has been calibrated against all available data sets for z ∼> 5 galaxies including the evolving UV luminosity function (UV LF) and stellar mass function (SMF)

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Summary

INTRODUCTION

Over the past decade instruments such as the Hubble Space Telescope (HST), Very large Telescope (VLT), Subaru and Keck have been used to assemble statistically large sample of high-redshift (z ∼> 5) Lyman break Galaxies (LBGs) at restframe ultra-violet (UV) wavelengths. Our goal is to: (i) study the key processes determining the dust content of high-redshift (z ∼> 7) LBGs; and (ii) explore the impact of different ISM grain-growth timescales on the dust masses and UV-observability of such galaxies To this end, we augment our delphi semi-analytic model with a detailed treatment of chemical and dust enrichment in the ISM of LBGs. similar in spirit to the semi-analytic models noted above (e.g. Popping et al 2017; Vijayan et al 2019; Triani et al 2020), the key strengths of this work lie in the fact that: (i) it uses a minimal number (two) of mass- and redshift-independent free parameters to model the key physics of early galaxies; (ii) contrary to the other models which have been calibrated against low-redshift (z ∼ 0 − 3) data, our model has been calibrated against all available data sets for z ∼> 5 galaxies including the evolving UV LF and SMF. While f∗ is crucial in determining the highmass end of the SMF, fw determines the low-luminosity and low-mass ends of the UV LF and SMF, respectively (Dayal et al 2014)

Modelling the dust and metal contents of high-redshift galaxies
Rate evolution of key dust processes
THE DUST CONTENT OF HIGH REDSHIFT GALAXIES
The impact of dust obscuration on the UV LF
The impact of dust obscuration on the UV-to-total star formation rate relation
Findings
CONCLUSIONS AND DISCUSSION
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