Study the spectral energy distribution (SED) of type 1 AGN in the optical, Near and Far-UV and X-ray...
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Transcript of Study the spectral energy distribution (SED) of type 1 AGN in the optical, Near and Far-UV and X-ray...
GALEX measurements of the Big Blue Bump as a tool to study bolometric corrections
Elena MarcheseR. Della Ceca, A. Caccianiga, P. Severgnini, A. Corral
Active Galactic Nuclei 9 – Ferrara , 24-27 May 2010
Study the spectral energy distribution (SED) of type 1 AGN in the optical, Near and Far-UV and X-ray energy bands .
Constrain the luminosity of the accretion disk emission component Derive the hard X-ray bolometric correction factors for a significant
sample of Type 1 AGN spanning a large range in z and Lx.
XXX
L
L
BH LdLLKc
zX
X
log)(1
)(max,
2
Accretion rate density
dzdz
dtzz
z
BHBH max
0
)()( Total accreted mass
Active Galactic Nuclei, powered by accretion onto a Super-massive Black Hole (SMBH), emit over the entire electromagnetic spectrum with the peak of the accretion disk emission in the far-UV, a wavelength range historically difficult to investigate.
The XMM-Newton Bright Survey in pills
XMM fields used: 237
Covered Area (deg2): 28
Sources in the bright sample(BSS,0.5-4.5keV): 389 “ “ “hard” bright sample(HBSS,4.5-7-5 keV): 67
(56 sources are in common)
Total Sources: 400 (fx >~7x10-14 erg cm-2 s-1)
Della Ceca et al., 2004Caccianiga et al., 2008
The starting point of our study is a sample of 304 AGNs, counting 263 type 1 AGNs having intrinsic NH <4 ·1021 cm-2, belonging to the
XMM-Newton Bright Serendipitous Survey (XBS).
GALEX (Galaxy Evolution Explorer) is a NASA Small Explorer mission that is performing surveys of different depths/sky coverage
in the far-UV and near-UV
The GALEX mission in pills
CROSS CORRELATION WITH GALEX
160 matches 63 upper limits
263 X-ray selected AGN 1, with NH <4 ·1021 cm-2
CROSS CORRELATION WITH SDSS
82 sources having data from XBS-GALEX-SDSS
The sample
All these sources have an X-ray spectra from XMM-Newton which allows us to derive X-ray luminosities and spectral properties (e.g. Γ, Nh).
• Corral, Della Ceca, Caccianiga and Severgnini, 2010, in preparation
• A. Corral:this meeting
40 sources out GALEX field
• The data points from the SDSS and from GALEX were described using a basic accretion disk model (DISKPN model in the XSPEC package). The maximum disc temperature was chosen in the range kT≈1-64 eV , and the normalization has been left has free parameter.
The model
Corrections to measured fluxes
Observer
Our Galaxy
Amm oss ,
VB
VV E
AR
AGN
Galactic reddening:Allen law(1976) Rv =3.1 EB-V = AB – AV available from the GALEX database
Intrinsic AGN reddeningThe exact shape of the extinction curve in the Near-Far-UV is still a matter of debate
Gaskell e Benker, 2007 determined a parametrized average extinction law from
the study of 14 AGN, with FUSE and HST data.
1221108.4
magcmE
N
VB
H
Bohlin et al. 1978
Host Galaxy
Hydrogen clouds (Lymanα forest)
Corrections to measured fluxes- IVOptical emission from the host galaxy
About 20% of the sources have optical SEDs showing a hardening at the optical wavelengths. Optical spectra of these sourcescontamination by the stars in the host galaxy
Break at 4000 Å : indicator of the importance of the galaxy star-light in the total emission of the source.
Calcium- break
F
FFF+ e F- mean flux densities in the regions 4050-4250
Å and 3750-3950Å (in the source rest-frame) respectively.
AGN
Host galaxy
AGN + host galaxy
Calcium break FL
UX
ENERGY (kev)
SDSS GALEX
SED OF ONE OF THE SOURCES
Model formulated to correct for the emission of the host galaxy
Model of a normal galaxy: Heaviside function such that Δ=50%
AGN: αν =-0.44 (αλ =-1.56).(Vanden Berk et al. 2001)
We calculated the resulting Δ from the combined emission of the AGN (with different normalizations) and host galaxy
FLU
X RA
TIO
AG
N/G
ALAX
Y
Break at 4000 Å
Ca break≈40%
HOST GALAXY
AGN
H.GALAXY+AGN
FLU
X
λ (Å)
HOST GALAXY
AGN
H. GALAXY+AGN
FLU
X λ (Å)Ca break≈2%
Corrections to measured fluxes- IVOptical emission from the host galaxy
HOST GALAXY
AGN
GAL+AGN
AGN
HOST GALAXY
GAL+AGN
Δ=17.3%
Δ=33.2%
0.
0.
ENERGIA (keV)
FLU
X FL
UX
ENERGY (keV)
ENERGY(keV)
SDSS
SDSS
GALEX
GALEX FLU
X FL
UX 0.
ENERGY (keV)
ENERGY (keV)
SDSS
SDSSGALEX
GALEX
AFTER CORRECTIONBEFORE CORRECTION
The presence of emission lines within the filter bandpass can contribute significantly to the observed magnitudes of an AGN. Since this effect is a strong function of redshift, we need to take it into account to derive the continuum…
Assuming R ~1
Average spectra and equivalent widths of the emission lines present in the energy bands we are studying, calculated by Telfer et al. 2002, from the spectra of 184 quasars with z>0.33 .
Corrections to measured fluxesEmission lines contribution
FLU
X
WAVELENGTH (Å)
TIPICAL SPECTRA OF AN AGN
FLUSSI OTTICO-UV
FLUSSI X
ENERGIA (keV)
FLUSSI OTTICO-UV
FLUSSI X
ENERGIA (keV)
FLUSSI OTTICO-UV
FLUSSI X
ENERGIA (keV)
OPTICAL-UV
X-rayXMM
ENERGIA (keV)
SPECTRAL ENERGY DISTRIBUTIONS
OPTICAL-UV
X-ray (XMM)
ENERGIA (keV)
Median maximum temperature : kT ≈ 4 eV
2-10 keV luminosityAvailable for every object from the X-ray spectral analysis (Corral et al. 2010)
0.1-100 keVluminosity Extrapolated from the 2-10 keV luminosity, using the spectal index measured for every sorce
Accretion disk luminosity
Calculated as the integral of the SEDs in the optical-UV bands.
L bol =L disc + L 0.1-100 keV
82 sources with XBS-GALEX-SDSS data discussed so far
78 sources with XBS-GALEX data
63 sources with XBS-GALEX upper limits
UV fluxes or their upper limits were fitted with the same model with a Tmax
fixed to kT ≈ 4 eV
Strong dependence of the accretion disk luminosities to the X-ray luminosities the
two emission mechanisms are highly correlated
Results - I CORRELATION LDISK – L2-10keV
Best-fit bisector relation:
913.8log)056.0232.1(log 102 keVdisc LL
In good agreement with previous results on X-ray selected sources: Lusso et al. 2010: β=1.31±0.038
78 sources XBS-GALEX
82 sources XBS-GALEX-SDSS
63 sources XBS-GALEX upper limits
keV
bolbol L
Lk
102
We don’t find any significant correlation between bolometrc
correction and X-ray luminosities
This is probably due to a very large spread in the distributions of
the hard X-ray bolometric corrections, going from ~5 up to few hundred, implying a large dispersion in the mean SED
Results - II BOLOMETRIC CORRECTION AGAINST HARD X-RAY LUMINOSITY
63 sources XBS-GALEX upper limits
78 sources XBS-GALEX
82 sources XBS-GALEX-SDSS
We used a sample of 223 sources spanning a large range in X-ray luminosities (LX ≈1041 – 1046 erg/s) and redshift (z≈0-2.4) and we find :
• A high correlation between the accretion disk luminosity and the X-ray luminosity, in agreement with previous works on X-ray selected AGNs.
• A very large spread in the distributions of the hard X-ray bolometric corrections, going from ~5 up to few hundred -> a large intrinsic dispersion in the mean SED;
Conclusions
Thank you