paper

HYPERION: broad-band X-ray-to-near-infrared emission of Quasars in the first billion years of the Universe

arXiv:2411.02105 · doi:10.1051/0004-6361/202450876

Abstract

We aim at characterizing the X-ray-to-optical/near-infrared broad-band emission of luminous QSOs in the first Gyr of cosmic evolution to understand whether they exhibit differences compared to the lower-\textit{z} QSO population. Our goal is also to provide for these objects a reliable and uniform catalog of SED fitting derivable properties such as bolometric and monochromatic luminosities, Eddington ratios, dust extinction, strength of the hot dust emission. We characterize the X-ray/UV emission of each QSO using average SEDs from luminous Type 1 sources and calculate bolometric and monochromatic luminosities. Finally we construct a mean SED extending from the X-rays to the NIR bands. We find that the UV-optical emission of these QSOs can be modelled with templates of 2 luminous QSOs. We observe that the bolometric luminosities derived adopting some bolometric corrections at 3000 Ã () largely used in the literature are slightly overestimated by 0.13 dex as they also include reprocessed IR emission. We estimate a revised value, i.e. which can be used for deriving in \textit{z} 6 QSOs. A sub-sample of 11 QSOs is provided with rest-frame NIR photometry, showing a broad range of hot dust emission strength, with two sources exhibiting low levels of emission. Despite potential observational biases arising from non-uniform photometric coverage and selection biases, we produce a X-ray-to-NIR mean SED for QSOs at \textit{z} 6, revealing a good match with templates of lower-redshift, luminous QSOs up to the UV-optical range, with a slightly enhanced contribution from hot dust in the NIR.

All photometric data and the derived properties (luminosities, spectral slopes) are available on Zenodo at https://zenodo.org/records/14867157 in machine-readable format. The repository also includes the mean SED template for QSOs at the Epoch of Reionization, as shown in Figure 13 of the paper