Journal
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 425, Issue 2, Pages 907-929Publisher
OXFORD UNIV PRESS
DOI: 10.1111/j.1365-2966.2012.21272.x
Keywords
accretion, accretion discs; galaxies: active
Categories
Funding
- Durham Doctoral Fellowship
- Alfred P. Sloan Foundation
- National Science Foundation
- US Department of Energy
- National Aeronautics and Space Administration
- Japanese Monbukagakusho
- Max Planck Society
- Higher Education Funding Council for England
- ESA Member States
- USA (NASA)
- STFC [ST/I001573/1, ST/G001588/1] Funding Source: UKRI
- Science and Technology Facilities Council [ST/G001588/1, ST/I001573/1] Funding Source: researchfish
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In this third paper in a series of three, we present a detailed study of the broad-band spectral energy distribution (SED) of active galactic nuclei (AGNs) based on a nearby unobscured type 1 AGN sample. We perform a systematic cross-correlation study of several key parameters, i.e. G2-10?keV, L2-10?keV, Lbol/LEdd = ?Edd, Lbol/L2-10?keV = ?2-10?keV, L bol /L5100 angstrom=?5100 angstrom, FWHMH beta, MBH, aox, aX and aUV. The well-defined spectral properties of the sample enable us to improve existing relations and to identify new correlations among these parameters. We confirm a break region around FWHMH beta ? 4000?km?s-1 in the G2-10?keV versus FWHMH beta correlation and log(MBH) ? 8.0 in the G2-10?keV versus MBH correlation, where these correlations appear to change form. Beyond the break point, the intrinsic G2-10?keV index is dispersed around 1.8. Several new correlations are also reported in this paper, e.g. strong correlations in ?5100 versus ?Edd, ?5100 versus ?2-10?keV and ?2-10?keV versus MBH. The principal component analysis (PCA) is performed on the correlation matrix of the above parameters. This shows that the three physical parameters, i.e. black hole mass, mass accretion rate and Eddington ratio, drive the majority of the correlations. This is consistent with PCA results found from previous optical spectral studies. For each key parameter, we split the AGNs into three subsamples, binned based on increasing value of that parameter. We co-add the model SEDs for each object in the subsample to see how the SED changes with that parameter. Most parameters, except Lbol, show similar systematic changes in the SED such that the temperature at which the disc peaks is correlated with the ratio of power in the disc versus the Comptonized components and the hard X-ray spectral index. This underlying change in SED shape shows that AGNs do exhibit intrinsically different spectral states. This is superficially similar to the SED differences in black hole binary (BHB) seen as ?Edd increases, but the analogy does not hold in detail. Only objects with the highest ?Edd appear to correspond to a BHB spectral state (the disc-dominated high/soft state). The AGNs with typical mass accretion rates have spectra which do not match well with any state observed in BHB. We speculate that this could be due to the presence of a powerful ultraviolet line-driven disc wind, which complicates simple mass scaling between stellar and supermassive black holes.
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