fabio la franca and n. sacchi, s. puccetti, f. fiore, c. gruppioni, c. feruglio et al

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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-S1 XMM/SWIRE/ELAIS-S1 Universita` degli Studi ROMA TRE

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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 Presentation

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Page 1: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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

Page 2: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

-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

Page 3: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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

Page 4: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

*) 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

Page 5: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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.

Page 6: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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

Page 7: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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

Page 8: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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

Page 9: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field SED classification of high MIR/O sources

Page 10: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field SED classification of high MIR/O sources

Page 11: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

Looking for absorbed AGN in the XMM/SWIRE/ELAIS-S1 field SED classification of high MIR/O sources

Page 12: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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…

Page 13: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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

Page 14: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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

Page 15: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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?

Page 16: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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

Page 17: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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

Page 18: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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

Page 19: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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

Page 20: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

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

Page 21: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

~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

Page 22: Fabio La Franca and  N. Sacchi, S. Puccetti, F.  Fiore, C. Gruppioni, C. Feruglio et al

-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