Publication Date:
2016-03-17
Description:
We present a detailed analysis of a recent, 2013 Suzaku campaign on the nearby ( z = 0.184) luminous ( L bol ~ 10 47 erg s –1 ) quasar PDS 456. This consisted of three observations, covering a total duration of ~1 Ms and a net exposure of 455 ks. During these observations, the X-ray flux was unusually low, suppressed by a factor of 〉10 in the soft X-ray band when compared to previous observations. We investigated the broad-band continuum by constructing a spectral energy distribution (SED), making use of the optical/UV photometry and hard X-ray spectra from the later simultaneous XMM–Newton and NuSTAR campaign in 2014. The high-energy part of this low-flux SED cannot be accounted for by physically self-consistent accretion disc and corona models without attenuation by absorbing gas, which partially covers a substantial fraction of the line of sight towards the X-ray continuum. At least two layers of absorbing gas are required, of column density log ( N H,low /cm –2 ) = 22.3 ± 0.1 and log ( N H,high /cm –2 ) = 23.2 ± 0.1, with average line-of-sight covering factors of ~80 per cent (with typical ~5 per cent variations) and 60 per cent (±10–15 per cent), respectively. During these observations PDS 456 displays significant short-term X-ray spectral variability, on time-scales of ~100 ks, which can be accounted for by variable covering of the absorbing gas along the line of sight. The partial covering absorber prefers an outflow velocity of $v_{\rm pc} = 0.25^{+0.01}_{-0.05}\,c$ at the 〉99.9 per cent confidence level over the case where v pc = 0. This is consistent with the velocity of the highly ionized outflow responsible for the blueshifted iron K absorption profile. We therefore suggest that the partial covering clouds could be the denser, or clumpy part of an inhomogeneous accretion disc wind. Finally estimates are placed upon the size-scale of the X-ray emission region from the source variability. The radial extent of the X-ray emitter is found to be of the order ~15–20 R g , although the hard X-ray (〉2 keV) emission may originate from a more compact or patchy corona of hot electrons, which is typically ~6–8 R g in size.
Print ISSN:
0035-8711
Electronic ISSN:
1365-2966
Topics:
Physics
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