Abstract

ALMA observations have revealed the presence of dust in the first generations of galaxies in the Universe. However, the dust temperature TdT_d remains mostly unconstrained due to the few available FIR continuum data at redshift z>5z>5. This introduces large uncertainties in several properties of high-zz galaxies, namely their dust masses, infrared luminosities, and obscured fraction of star formation. Using a new method based on simultaneous [CII] 158μμm line and underlying dust continuum measurements, we derive TdT_ d in the continuum and [CII] detected z≈7z\approx 7 galaxies in the ALMA Large Project REBELS sample. We find 39 K<Td<58 K39\ \mathrm{K} < T_d < 58\ \mathrm{K}, and dust masses in the narrow range Md=(0.9−3.6)×107M⊙M_d = (0.9-3.6)\times 10^7 M_{\odot}. These results allow us to extend for the first time the reported Td(z)T_d(z) relation into the Epoch of Reionization. We produce a new physical model that explains the increasing Td(z)T_ d(z) trend with the decrease of gas depletion time, tdep=Mg/SFRt_{dep}=M_g/\mathrm{SFR}, induced by the higher cosmological accretion rate at early times; this hypothesis yields Td∝(1+z)0.4T_d \propto (1+z)^{0.4}. The model also explains the observed TdT_d scatter at a fixed redshift. We find that dust is warmer in obscured sources, as a larger obscuration results in more efficient dust heating. For UV-transparent (obscured) galaxies, TdT_d only depends on the gas column density (metallicity), Td∝NH1/6T_d \propto N_H^{1/6} (Td∝Z−1/6T_d \propto Z^{-1/6}). REBELS galaxies are on average relatively transparent, with effective gas column densities around NH≃(0.03−1)×1021cm−2N_H \simeq (0.03-1)\times 10^{21} \mathrm{cm}^{-2}. We predict that other high-zz galaxies (e.g. MACS0416-Y1, A2744-YD4), with estimated Td≫60T_d \gg 60 K, are significantly obscured, low-metallicity systems. In fact TdT_d is higher in metal-poor systems due to their smaller dust content, which for fixed LIRL_{ IR} results in warmer temperatures.

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