Fig. 7.

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Observed [C II]/[C I] luminosity line ratio, as a function of the CO(7–6)/IR luminosity ratio (left panel), for the quasars in our study (filled circles; see references in the main text), as well as other high redshift (z > 1) galaxies and quasar hosts (filled squares) and local galaxies (empty stars, based on Rosenberg et al. 2015). All the quasars in our study show [C II]/[C I] ratios ≳20, which are not compatible with XDRs. Our sample also displays a range of CO(7–6)/IR ratios comparable with other high–z sources, but a factor ∼2−3× higher than the bulk of the local galaxies. Right: predictions of the [C II]/[C I] ratio as a function of the CO(7–6)/IR luminosity ratio for various gas densities log nH[cm−3] = (3, 4, 5) for a PDR with incident radiation field log G0 = (2, 3, 4) and an XDR with log FX = ( − 1, 0, +1). Our sources (shown in filled circled, with the same color scheme as in the left-hand panel) are best described by a PDR–like environment with NH ∼ 1023 cm−2, nH ≳ 104 cm−3, and G0 ∼ 103.
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