fabio la franca and n. sacchi, s. puccetti, f. fiore, c. gruppioni, c. feruglio et al
DESCRIPTION
The nature and density of Spitzer selected X-ray absorbed AGN: Identification of sources with large MIR/Optical ratios in the XMM/SWIRE/ELAIS-S1. Fabio La Franca and N. Sacchi, S. Puccetti, F. Fiore, C. Gruppioni, C. Feruglio et al. Dipartimento di Fisica. Universita` degli Studi ROMA TRE. - PowerPoint PPT PresentationTRANSCRIPT
Fabio La Franca
and N. Sacchi, S. Puccetti, F. Fiore, C. Gruppioni, C. Feruglio
et al.
Dipartimento di Fisica
The nature and density of Spitzer selected X-ray absorbed AGN:
Identification of sources with large Identification of sources with large MIR/Optical ratios in the MIR/Optical ratios in the XMM/SWIRE/ELAIS-S1XMM/SWIRE/ELAIS-S1
Universita` degli Studi ROMA TRE
-What is the fraction of AGN among the sources with large MIR/O?
-What is the fraction of absorbed AGN?
-Is the density of absorbed AGN compatible to other estimates orextrapolations (i.e. XLF)?
QUESTIONSQUESTIONS
What do we know about the AGN evolution?
A Luminosity Dependent Density Evolution(LDDE) for X-ray AGN isobserved(e.g. Ueda+03; Fiore+03; La Franca+05;Barger+05; Hasinger+05; Gilli+07; Silverman+07; Della Ceca+08)
Lower luminosity AGNpeak at lower redshifts:DOWNSIZING(see models of galaxy andAGN formations)
La Franca+05
*) Assuming no luminosity and redshift dependences
assumed *)
expected
What do we know about the AGN evolution?
The fraction of absorbed AGN as function of LX and z
DECREASE WITH LUMINOSITYEarlier evidences of a decrease of the fraction of absorbed AGN with luminosity from Lawrence & Elvis (1982), confirmed by Ueda et al. (2003).
INCREASE WITH THE REDSHIFT
Fract
ion o
f A
bso
rbed A
GN
La Franca+05
The LX-z plane
~1x10-15@2Ms
?
X-ray stacking analysis of MIR selected AGNsX-ray stacking analysis of MIR selected AGNsallows to probe more distand, more absorbed,allows to probe more distand, more absorbed,lower luminosity, regions of the Llower luminosity, regions of the LXX-N-NHH-z plane-z plane
Many studies indicate that the majorityof the sources with extremeF(24um)/F(R) (e.g. >1000) ratios areobscured/absorbed AGNs
(see e.g. Martinez-Sansigre+05; Houck+05;Weedman+06; Brown+06; Polletta+06; Yan+07; Daddi+07; Fiore+08; Georgantopoulos+08…)
However,1) these sources are so faint, that direct optical spectroscopic classifications
is available for very few of them;2) the density estimates are based on assumptions on the NH distribution.
AREA0.6 deg2 (:0.5h, :-43.5o)
IMAGINGBVRIz (PI Franceschini; Berta+06+08)
JK (PI Cimatti/Maiolino; Dias+08)
SWIRE (PI Lonsdale & Rowan-Robinson)(3.6, 4.5, 5.8, 8.0 and 24 μm)
X-ray (PI: Fiore) by XMM 4x100Ks (Puccetti+06)
Chandra x5 (Puccetti in prep)
SPECTROSCOPY(PI La Franca; Sacchi in prep)
~100 hours withVIMOS and FORS2@VLT
Total~1500 Zs (R<24.5) (K, 3.6um and 24um sources)
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field Method: data
Catalogue of ~1700 24m sources with F24 > 0.280 mJy
Redshift for 384 sources with R<24.2
Seyfert2/AGN2 (SED:10-13) Seyfert2/AGN2 (SED:10-13)
ULIRG/Starburst (SED: 7-9)ULIRG/Starburst (SED: 7-9)
Spirals Star Forming (SED:14-20)Spirals Star Forming (SED:14-20)
Ellipticals (SED:21)Ellipticals (SED:21)
Red Power Law ~AGN1 (SED:1-6) Red Power Law ~AGN1 (SED:1-6)
Adapted from Polletta et al. (2007)
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field Method: SED templates fitting
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field Method: SED templates fitting
(see Polletta et al. 2007)
AGN2
AGN1
Normal
χ2 best fit analysis
1st choice
2nd choice 3rd choice
SED
Normal
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field SED classification of high MIR/O sources
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field SED classification of high MIR/O sources
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field SED classification of high MIR/O sources
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field SED classification of high MIR/O sources
Local relationshipun-absorbed AGN
20%20%
4343%34%34%
3%3%
What is the fraction/densityof (possibly absorbed) AGNamong these high MIR/Osources?
First look at the OPT spectra…
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field OPTICAL VLT SPECTROSCOPY of faint (R>22) high MIR/O sources
TOTAL: 384 spectra
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field OPTICAL VLT SPECTROSCOPY of faint (R>22) high MIR/O sources
composite spectraTOTAL: 384 spectra
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field OPTICAL VLT SPECTROSCOPY of faint (R>22) high MIR/O sources
82% of SED-PWL are optical 82% of SED-PWL are optical AGNAGN93% of SED-ULIRG are optical 93% of SED-ULIRG are optical ELGELGSED-Seyfert2: no preferencesSED-Seyfert2: no preferences
composite spectraTOTAL: 384 spectra
40% AGN2 (& AGN1)
60% ELG
56 spectra
What about their SED?
X-ray detections and stacking (filled symbols)
STACKED DATA
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field X-ray stacking analysys of faint (R>22) high MIR/O sources
82% of OPT-AGN82% of OPT-AGNare X-ray absorbed AGNare X-ray absorbed AGN
85% of OPT-ELG85% of OPT-ELGare mildly X-ray are mildly X-ray absorbed withabsorbed withLL2-102-10~10~1041-4241-42
MID TERM SUMMARY:SED-PWL --> optical AGN(2) --> X-ray absorbed AGNSED-ULIRG --> optical ELG --> mildly absorbed low LX
Spec. and phot. redshiftsSpec. and phot. redshifts
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field SED classification of high MIR/O sources
The sources with F24/FR>120 havez>0.6 and LogL24>44
Analysis for ∆z=0.6-1.3*
i.e.∆LogL24=44-45.5
*) At z>1.3 the sample is incomplete becouse of fainter R>25 unindentified sources
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field X-ray properties of low MIR/O sources
X-ray detections and stacking (filled symbols)
Low MIR/O sources show low LX and mild absorption,compatible with absorbed X-ray spectra of strongstar-forming galaxies
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field X-ray properties of high MIR/O sources
X-ray detections and stacking (filled symbols)
SOFT0.3-1.5 keV
HARD1.5-6 keV
R>25
SED-SEY2
SED-Red PWL
What are their densities?…
73% of large MIR/O (F24/R>120) sources are absorbed AGN
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field Density of X-ray absorbed large MIR/O sources
The density is compatible with the extrapolations
coming from previous estimates at z~1of the XLF of Compton thin AGN
LogNH~22.3
LogNH~23.1
~1x10-15@2Ms
Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field Density of X-ray absorbed large MIR/O sources
?
We have probed a one decade less luminous region at z~1 or a 0.7 larger redshift at LogL2-10~42.5
-We have carried out optical spectroscopic identification of 56 sourceswith F24/R>120 and R<24.2.
- The fraction of optically classifiedoptically classified (or X-ray luminous) AGN is 40(45)%. SED-PWL --> optical AGN(2) --> X-ray absorbed AGN SED-ULIRG --> optical ELG --> mildly absorbed, low LX
-According to the X-ray stacking analysis, 73% of the sources are absorbed(22<LogNH<23.5) AGN with Log(L2-10)>42 cgs.
-Their density is compatible with the extrapolations at z~1 of the XLFof Compton thin AGN.
SUMMARY