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Evolution of Supermassive Black Holes from deep & large area X-ray surveys Marcella Brusa (Max Planck Institut fuer Extraterrestrische Physik)
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AGN 8 - Torino, May 2008 Outline Introduction: AGN evolution What we know: observations & models Still missing (among others..): high-redshift population Compton Thick AGN census Summary & future
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AGN 8 - Torino, May 2008 Main actors in this game XMM/Chandra COSMOS teams CDFS/GOODS/MUSIC team ELAIS-S1 team HELLAS2XMM team.. and in particular thanks to: A.Comastri, F.Fiore, R.Gilli, A.Bongiorno, N.Cappelluti, F.Civano, G.Hasinger, K. Iwasawa, V. Mainieri, A. Merloni, M. Mignoli, S.Puccetti, M.Salvato, C. Vignali, G.Zamorani, C.Feruglio, A.Grazian, F.LaFranca, F.Pozzi, P.Santini…
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AGN 8 - Torino, May 2008 introduction AGN evolution Once upon a time… (1960s-70s): QSO/AGN are triggered by accretion on SMBH QSO/AGN are 1% of galaxy population: transient phase or rare objects? [45 years of observations] Nowadays: SMBH can be revealed in almost 100% of local galaxies AGN transient phase!
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AGN 8 - Torino, May 2008 MAIN OBSERVATIONAL RESULT: The discovery of dead SMBH in most local bulges & tight correlation between M BH and bulge properties Co-evolution of galaxies and SMBH Large scale Galaxy properties strongly depend on BH mass Ferrarese & Merritt 2000 Gebhardt et al. 2000 Marconi & Hunt 2003
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AGN 8 - Torino, May 2008 AGN and galaxy co-evolution Early on Strong galaxy interactions; Mergers between gas rich galaxies drive gas which fuel both SF and BH activity; Violent starbursts episodes; Heavily obscured BH growth When galaxies coalesce A ccretion peaks; SMBH becomes optically “visible” (QSO phase) as AGN winds blow out gas Later times SF & BH accretion quenched; Dead quasars (or slowly accreting BH) in red galaxies (passive evolution) [see also Granato+2004, Di Matteo, Springel & Hernquist 05, Hopkins+07] Li et al. 2007 To prove this scenario we need: 1)Complete SMBH census, 2)Physical models for AGN feedbacks 3)Observational constraints to these models Li et al. 2007
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AGN 8 - Torino, May 2008 How to study AGN evolution? Count and detect AGN at different phase/stages of their evolution Surveys Accretion Luminosity is emitted over a broad range of wavelengths, BUT the X-ray emission is the AGN footprint X-ray surveys AGN come in 2 flavours: unobscured and obscured,obscuration affects mostly the soft X-ray and optical wavelengths Hard (>2 keV) X-ray surveys (unbiased) Multiwavelength follow-up (redshifts!)
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AGN 8 - Torino, May 2008 Evolution of Obscured AGN – why bother? (1) XRB fit Gilli, Comastri, Hasinger 07 Red -> unobscured AGN Blue + Black -> obscured AGN Obscured AGN are needed to reproduce the XRB peak [e.g. Setti & Woltjer 1989 ……. Gilli, Comastri & Hasinger 2007]
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AGN 8 - Torino, May 2008 IF all galaxies undergo an AGN phase and IF dead SMBH observed today are the remnants/witnesses of this phase The BH mass density obtained integrating the luminosity emitted by AGN over the cosmic time is expected to be similar to that measured in local bulges Soltan’s argument: mass accreted is equal to the energy released (E = mc 2 …) (Soltan 1982) ρ(direct) ~ ρ ● ~ 3-5.5 x 10 5 M ⊙ Mpc -3 [see e.g. Shankar et al. 2008 Marconi et al. 2004, Fabian 2003, Fabian & Iwasawa 1999 etc] Evolution of Obscured AGN – why bother? (2) BH growth INCLUDING ALSO OBSCURED / CT AGN
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AGN 8 - Torino, May 2008 XMM-COSMOS 2 deg2 -16 -15 -14 -13 Flux 2-10 keV (cgs) CDFN-CDFS 0.1deg2 Barger et al. 2003; Szokoly et al. 2004 EGS/AEGIS 0.5deg2 Nandra et al. 2006 HELLAS2XMM 1.4 deg2 Fiore et al. 20003 Cocchia et al. 2006 Champ 1.5deg2 Silverman et al. 2005 XMM HBS ~25 deg2 Della Ceca+04,08 XBOOTES 9 deg2 Murray et al. 2005, Brand et al. 2005 Survey of surveys - X-rays + multiwave SEXSI 2 deg2 Eckart et al. 2006 Area (see Brandt & Hasinger 2005 ARA&A 43, 827) E-CDFS 0.3deg2 Lehmer et al. 2005 ELAIS-S1 0.5deg2 Puccetti et al. 06, Feruglio et al. 08 Lockman Hole 0.2 deg2 Brunner et al. 2008 Contiguous C-COSMOS 0.9 deg2
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AGN 8 - Torino, May 2008 picture quite clear from optical/soft/hard X-ray surveys: Luminosity-Dependent Density Evolution (LDDE) [see also Ueda+03, Cirasuolo+05, Della Ceca+08] Anti-hierarchical growth/Downsizing [Cowie et al. 1996, Merloni 2004, De Lucia et al. 2006] Evolution Fiore +03 La Franca +05 Hasinger+05 Bongiorno+07
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AGN 8 - Torino, May 2008 Fraction of absorbed sources: Luminosity dependence fraction of obscured AGN is a strong function of L: most luminous, less obscured Same result in DIFFERENT bands despite the very different selections!! Hasinger et al. 2005 (see also La Franca +05, Treister+05, Della Ceca+08) Black: X-ray Hasinger 2008 Green: IR Maiolino et al. 2007 Red: Optical Simpson et al. 2005
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AGN 8 - Torino, May 2008 Fraction of absorbed sources: Redshift dependence more debated! Seen in (some) data [e.g. La Franca+05, Treister+06, Hasinger08], not seen in others (Ueda+03, Dwelly&Page 2006), not needed in XRB models (Gilli+07) but expected/predicted in feedback models (Menci+08) La Franca +05 Hasinger 2008
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AGN 8 - Torino, May 2008 Still missing (open problems) Compton Thick objects / census number density and evolution of high-z population (z>3) Interplay between AGN and SF / feedback models [see Marulli/Fontanot] Bolometric output/reprocessing [see Severgnini/Bellocchi/Lusso] BH mass / accretion rate evolution [see Labita] Elusive AGN (e.g. XBONGs/EXOs) [see Civano/Del Moro/Lanzuisi] Role of the envinronment in triggering nuclear activity [e.g. results from AEGIS/Groth strip – Georgakakis+07,08]
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AGN 8 - Torino, May 2008 The population of z>3 QSOs (XMM-COSMOS) Brusa, Comastri, Gilli et al. 2008, ApJ, submitted
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AGN 8 - Torino, May 2008 ? The population of z>3 QSO Radio QSO (Wall et al., 2005) Optical QSOs (Schmidt et al., 1995, Fan et al. 2001,2004) X-ray: What happens at z>3? decline or ~costant ? Soft X-ray ROSAT/Chandra/ XMM (Hasinger, Miyaji & Schmidt 2005) Chandra/ROSAT (Silverman et al. 2005/2007) statistics still low at z~3-5 (NO statistics at z>6) COSMOS
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AGN 8 - Torino, May 2008 + MAMBO, CFHT, Bolocam and (future) others COSMOS major components (in order of appearance) : HST/ACS (I-band – 590 orbits – I(AB)~27) 2002-2003: Subaru imaging (~25 nights - b,v,r,i,z=26/27) VLA (265 hours – 24 μJy) GALEX deep (200 ks, AB~25) XMM-Newton (800 ks – 10 -15 cgs) 2004-2005: XMM-Newton (600 ks) VLT (540 hours) & Magellan (12+ nights) SPITZER-IRAC (200 hours - ~1 μJy) 2006: SPITZER-MIPS (200 hours - ~70 μJy ) Chandra (1.8 Ms) Cosmos Survey 2 deg 2 (PI: N. Scoville) >150 team members worldwide! http://www.astro.caltech.edu/cosmos/ XMM-Newton PI: G. Hasinger Hasinger et al. 2007 soft 0.5-2.0 keV medium 2.0-4.5 keV hard 4.5-10.0 keV http://cosmos.astro.caltech.edu ApJS special issue vol. 172 (>550 pages!)
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AGN 8 - Torino, May 2008 AGN redshift distribution in XMM-COSMOS X-ray sample (AGN) Empty: specz+photz Filled: specz Sources extracted from a flux limited sample in XMM-COSMOS (50% of the area coverage in at least one band) 1651 XMM sources - 10% problematic ID using IR+Chandra info ~670 “secure” spectroscopic redshifts (40%), incompleteness especially for high-z and Type 2 AGN Accurate photometric redshifts available (Salvato et al. 2008)
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AGN 8 - Torino, May 2008 LESS than 10% catastrophic outliers (to be compared with COMBO-17, Wolf et al. 2004) 434 objects with “super-secure” spectro-z (further refinement/analysis) Photo-z computed using >30 bands: SDSS, Subaru including IB, CFHT, J, K, IRAC.. AGN photometric redshifts Salvato et al. (in prep)
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AGN 8 - Torino, May 2008 AGN redshift distribution in XMM-COSMOS X-ray sample (AGN) Empty: specz+photz Filled: specz z>3 sample: 40 objects (22 specz + 18 photoz) Additional 14 objects, no photoz available. Candidates very high-z AGN (EXOs, Koekemoer et al. 2004) Sources extracted from a flux limited sample in XMM-COSMOS (50% of the area coverage in at least one band) 1651 XMM sources - 10% problematic ID using IR+Chandra info ~670 “secure” spectroscopic redshifts (40%), incompleteness especially for high-z and Type 2 AGN Accurate photometric redshifts available (Salvato et al. 2008)
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AGN 8 - Torino, May 2008 Examples of images, spectra & photoz B g v r I z IRAC 3.6 XID 54439 z=4.241
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AGN 8 - Torino, May 2008 X-ray properties HR vs. redshift Ratio of obscured/ unobscured objects in agreement with XRB models
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AGN 8 - Torino, May 2008 Contribution to source counts Lower bound: 22 spectro-z Upper-bound: adding 10 EXOs Dashed line: Expectations from XRB models using Hasinger et al. 2005 LF Solid line: Exponential decay introduced at z=2.7 (Schmidt+95) Flat evolution completely ruled out Tightest constraints to date (largest and cleanest sample) z>4 point : Rhook & Haenelt 08 predict a factor of ~3 higher wrt data Models: Gilli, Comastri & Hasinger 2007, A&A
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AGN 8 - Torino, May 2008 Space densities Red curve: predictions from XRB models logLx>44.2 AGN (unobs+obs) [Gilli+07 using Hasinger+05 and La Franca+05] Dashed area: (rescaled) space density for optically selected bright QSO [Richards+2006, Fan+2001] Blue curve: Silverman+08 LF, I<24 sample
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AGN 8 - Torino, May 2008 The census of z~1-3 CT AGN/QSOs (CDFS+COSMOS) Fiore et al. 2008a, ApJ, 672, 94 Fiore, Puccetti, Brusa et al. 2008b, ApJ, submitted
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AGN 8 - Torino, May 2008 Unveiling obscured accretion X-ray surveys : miss most highly obscured (Compton Thick) AGN [e.g. Comastri 2004, Worsley et al. 2005] IR surveys : highly obscured AGN shine in the MIR – dust reprocessing [e.g. Martinez-Sansigre et al. 2005, Polletta et al. 2006] Goal: combining X-ray and IR surveys to get the SMBH census and compile AGN bolometric LF X-ray-MIR surveys: CDFS/GOODS/MUSIC [Grazian et al. 2006, Brusa et al. in prep, CDFS team papers] ELAIS-S1/SWIRE [Feruglio et al. 2008, La Franca et al. 2008] COSMOS [XMM-COSMOS: Brusa et al. 2008; + C-COSMOS/S-COSMOS papers] X-ray surveys : miss most highly obscured (Compton Thick) AGN [e.g. Comastri 2004, Worsley et al. 2005] IR surveys : highly obscured AGN shine in the MIR – dust reprocessing [e.g. Martinez-Sansigre et al. 2005, Polletta et al. 2006] Goal: combining X-ray and IR surveys to get the SMBH census and compile AGN bolometric LF X-ray-MIR surveys: CDFS/GOODS/MUSIC [Grazian et al. 2006, Brusa et al. in prep, CDFS team papers] ELAIS-S1/SWIRE [Feruglio et al. 2008, La Franca et al. 2008] COSMOS [XMM-COSMOS: Brusa et al. 2008; + C-COSMOS/S-COSMOS papers]
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AGN 8 - Torino, May 2008 All sources BL AGN NOT BL AGN High MIR/O MIR selection of CT AGN XMM-COSMOS sample HR distribution [Brusa et al. 2008b] See also results from ELAIS-S1, Feruglio et al. 2008, Lanzuisi’s talk Select candidate, luminous obscured AGN by imposing: 24 micron bright fluxes (luminous) + optically faint red sources (optically obscured) high MIR/O ratio Select candidate, luminous obscured AGN by imposing: 24 micron bright fluxes (luminous) + optically faint red sources (optically obscured) high MIR/O ratio
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AGN 8 - Torino, May 2008 Combining MIR/O and R-K criteria: selection of CT AGN at z~2 Fiore et al. 2008a See also Daddi et al. 2007 GOODS CDFS field (1 Ms Chandra data) + MUSIC MW catalog (Spitzer+HST+VLT) ~110 obscured AGN candidates Stack of Chandra images excluding X-ray detections in two different MIR/O and R-K bins Tracks of obscured AGN [Pozzi et al 2007]
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AGN 8 - Torino, May 2008 A new population of CT AGN Curves: model predictions from Gilli, Comastri & Hasinger (2007) for L> 42, 43, 44, 45 Daddi et al. 2007 Fiore et al. 2008 Martinez-Sansigre et al. 2005 Polletta et al. 2006 The observed MIR luminosity and the observed HR imply (unobs) Lx>43 and NH>24 for ~80% of the sources Low R-K or
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AGN 8 - Torino, May 2008 COSMOS MIR AGN Fiore et al. 2008b High AGN fraction (~65%) in MIPS selected samples (deeper X-ray data + more comprehensive analysis)
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AGN 8 - Torino, May 2008 Summary The fraction of obscured sources depend strongly on luminosity The fraction of obscured sources evolves (increases) with redshift Flat evolution at z>3 definitively ruled out (space densities & number counts) Significant population of CT QSO at z~2 detected
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AGN 8 - Torino, May 2008 What’s next? Compton Thick AGN/quasars: XMM ultra deep 1.3 Ms (this fall) exploit stacking… (Chandra 2 Ms) Simbol-X (high-energy) Herschel (reprocessing) High-z quasars: eROSITA (high-L) XEUS (low-L and very high-redshift) joint multiwavelength campaigns
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