Fig. 6.

Estimated upper limits (ΔC = 3.84, equivalent to the 95% confidence level in the Gaussian approximation) on the column density NH(z) as a function of the observed hardness ratio for each source of our sample. Such constraints are obtained from the spectral fits with an absorbed power-law model, where an intrinsic continuum with Γ = 1.8 was adopted for the faintest objects (red symbols). The synthetic NH(z)–HR curves corresponding to an absorbed spectrum with Γ = 2.0 (black) and 1.5 (magenta) are also plotted for reference. These have been computed for the mean Galactic column ( cm−2) and quasar redshift (z = 3.14), assuming the energy-dependent response of the pn detector. The grey and lilac shaded areas respectively illustrate the uncertainties due to the full range of
and z covered by the sample. The large majority of our objects are consistent with being, at most, mildly obscured (i.e. NH < a few ×1022 cm−2).
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