2012MNRAS.425..907J


Query : 2012MNRAS.425..907J

2012MNRAS.425..907J - Mon. Not. R. Astron. Soc., 425, 907-929 (2012/September-2)

A combined optical and X-ray study of unobscured type 1 active galactic nuclei – III. Broad-band SED properties.

JIN C., WARD M. and DONE C.

Abstract (from CDS):

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. Γ2–10keV, L2–10keV, Lbol/LEdd= λEdd, Lbol/L2–10keV= κ2–10keV, \mi L\mi bol\mo/\mi L\mn 5100\mspaceAAkappa\mn 5100\mspaceAA, FWHMHβ, MBH, αox, αX and αUV. 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 FWHMHβ ≃ 4000km/s in the Γ2–10keV versus FWHMHβcorrelation and log(MBH) ≃ 8.0 in the Γ2–10keV versus MBH correlation, where these correlations appear to change form. Beyond the break point, the intrinsic Γ2–10keV index is dispersed around 1.8. Several new correlations are also reported in this paper, e.g. strong correlations in κ5100 versus λEdd, κ5100versus κ2–10keV and κ2–10keV 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 λEdd increases, but the analogy does not hold in detail. Only objects with the highest λEdd 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.


Abstract Copyright: 2012 The Authors Monthly Notices of the Royal Astronomical Society 2012 RAS

Journal keyword(s): accretion, accretion discs - galaxies: active

Simbad objects: 9

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Number of rows : 9
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 LBQS 0109+0213 QSO 01 12 16.9871883144 +02 29 47.691927816   17 17.8     ~ 43 0
2 LEDA 26550 Sy1 09 22 47.0337452784 +51 20 37.977167616   17.89 17.56     ~ 90 1
3 Mrk 110 Sy1 09 25 12.8479065576 +52 17 10.386311208   16.82 16.41     ~ 681 1
4 4C 13.41 Sy1 10 07 26.0965408440 +12 48 56.184940764   15.81 15.68     ~ 418 2
5 6C 102810+311911 BLL 10 30 59.0936990784 +31 02 55.723145964   17.07 16.71 16.1   ~ 192 1
6 ICRF J151443.0+365050 Sy1 15 14 43.0683049560 +36 50 50.355436776   17.11 17.01 15.83   ~ 422 1
7 2E 3542 Sy1 15 58 29.3628222264 +27 17 14.202585888   17.67 17.37     ~ 39 1
8 Mrk 509 Sy1 20 44 09.7504483224 -10 43 24.727155528   13.35 13.12 10.7   ~ 1370 0
9 2MASS J22360767+1343554 Sy1 22 36 07.6824548136 +13 43 55.360914636   16.48 16.34     ~ 170 0

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