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The multiwavelength surveys of the ELAISS1 and GOODS fields

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Strong constraints to models for the formation and evolution of structure in the Universe ... Miss most highly obscured AGN. La Franca et al. 2005. 2-10 keV ... – PowerPoint PPT presentation

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Title: The multiwavelength surveys of the ELAISS1 and GOODS fields


1
The multiwavelength surveys of the ELAIS-S1 and
GOODS fields
Fabrizio Fiore M. Brusa, A. Comastri, C.
Feruglio, A. Fontana, A. Grazian, F. La Franca,
P. Santini, E. Piconcelli, S. Puccetti and many
others
2
GOAL
  • AGN Bolometric Luminosity function
  • Complete SMBH census
  • Strong constraints to models for the formation
    and evolution of structure in the Universe

3
Co-evolution of galaxies and SMBH
  • Two seminal results
  • The discovery of SMBH in the most local bulges
    steep and tight correlation between MBH and bulge
    properties.
  • The BH mass density obtained integrating the AGN
    L.-F. and the CXB that obtained from local
    bulges

? most BH mass accreted during luminous AGN
phases! Most bulges passed a phase of
activity Need to understand AGN physics and
evolution to fully understand galaxy evolution
4
Why multiwavelength surveys
  • X-ray surveys
  • very efficient in selecting unobscured and
    moderately obscured AGN
  • Miss most highly obscured AGN

La Franca et al. 2005
5
2-10 keV AGN luminosity function models
Solid observed dashed best fit
LDDE with constant NH distribution
La Franca et al.
2005
6
Highly obscured Mildly Compton
thick INTEGRAL survey 100
AGN Sazonov et al. 2006
7
2-10 keV AGN luminosity function models
2-10keV 0.5-2keV
LDDE with variable absorbed AGN fraction La
Franca et al. 2005, see the poster by Fabio La
Franca
8
A working scenario
small mass progenitors. Feedback is effective in
self-regulating accretion and SF, cold gas is
left available
Galactic cold gas available for accretion and
obscuration increases at high z
Menci hierarchical clustering model, Menci,
Puccetti Fiore 2006
large mass progenitors. Feedback is less
effective, most gas is quickly converted in stars
at high z.
9
  • 1) Paucity of Seyfert like sources _at_ zgt1 is real?
    Or, is it, at least partly, a selection effect?
  • Are we missing in Chandra and XMM surveys highly
    obscured (NH?1024 cm-2) AGN? Which are common in
    the local Universe

10
Why multiwavelength surveys
  • IR surveys
  • AGNs even highly obscured at optical and X-ray
    energies shine in the MIR
  • Very difficult to isolate AGN from passive and
    starforming galaxies (Lacy 2004, Barnby 2005,
    Stern 2005, Polletta 2006 and many others)

Polletta et al. 2006
11
Why multiwavelength surveys
  • Use both X-ray and MIR surveys
  • Select unobscured and moderately obscured AGN in
    X-rays
  • Add highly obscured AGNs selected in the MIR
  • Simple approach Differences are emphasized in a
    wide-band SED analysis

12
X-ray-MIR surveys
  • CDFS-Goods MUSIC catalog (Grazian et al. 2006).
    Area 0.04 deg2
  • 173 X-ray sources, 104 2-10 keV down to 3?10-16
    cgs, 109 spectroscopic redshifts
  • 4300 MIPS sources down to 6.8 ?Jy, 3.6?m
    detection down to 0.08 ?Jy
  • Ultradeep Optical/NIR photometry, R27.5, K24
  • ELAIS-S1 SWIRE/XMM/Chandra survey (Puccetti et
    al. 2006, Feruglio et al. 2006). Area 0.5 deg2
  • 500 sources, 205 2-10 keV down to 3?10-15 cgs,
    half with spectroscopic redshifts.
  • 2600 MIPS sources down to 100 ?Jy, 3.6?m
    detection down to 6 ?Jy
  • Relatively deep Optical/NIR photometry, R25,
    K19
  • In future we will add
  • COSMOS XMM/Chandra/Spitzer. Area 2 deg2 see
    Marcella talk
  • CDFN-Goods. Area 0.04 deg2
  • Etc.

13
MIR selection
CDFS obs. AGN ELAIS-S1 obs. AGN
GOODS 24?m galaxies ELAIS-S1 24?m
galaxies Open symbols unobscured AGN Filled
symbols optically obscured AGN
14
MIR selection
CDFS obs. AGN ELAIS-S1 obs. AGN
GOODS 24?m galaxies
15
MIR AGNs
16
F24?m/FR gt1000 R-Kgt4.5
F(0.3-1.5keV)10-17 cgs
F(1.5-4keV)10-17 cgs
17
F24?m/FR gt1000 R-Kgt4.5
  • 119 sources (3 of the MIPS sample)
  • 17 detected by Chandra (9 2-10 keV band) 4 more
    visible in the image ltLXgt43.45/-0.24,
    ltNHgt22.9/-0.8, ltzgt2.1
  • logF(1.5-4keV) stacked sources-17
  • _at_z2 logLobs(2-8keV) stacked sources 41.8
  • logltLIRgt44.6 gt logL(2-8keV) unabs.43
  • Difference implies logNH?24
  • ltSFR-IRgt400!!
  • Msun/yr
  • ltSFR-UVgt5!!
  • Msun/yr
  • ltSFR-Xgt65
  • Msun/yr

18
F24?m/FR gt1000 R-Kgt4.5
19
F24?m/FR lt100 R-Kgt4.5
F(0.3-1.5 keV)2?10-17 cgs
F(1.5-4 keV) lt 5?10-18 cgs
20
F24?m/FR lt100 R-Kgt4.5
  • 125 sources (3 of the MIPS sample)
  • 29 detected by Chandra, 19 2-10 keV,
    ltLXgt43.4/-0.4 ltNHgt23.2/-0.6, ltzgt1.4
  • ltSFR-IRgt 8 Msun/yr
  • ltSFR-UVgt 2.6 Msun/yr
  • ltSFR-Xgt20 Msun/yr

21
Summary
  • XMM Chandra surveys can probe unobscured and
    moderately obscured accretion up to z2-4
  • INTEGRAL/Swift find highly obscured AGN up to
    z0.1
  • Spitzer finds highly obscured AGN at z1-3
  • Herschel will further increase the band, so
    helping in separating AGN from normal galaxies
    and pushing toward higher z.
  • During the next decade highly obscured AGN will
    be confirmed and studied in detail using hard
    X-ray focusing telescopes.
  • All this will allow a precise determination of
    the evolution of the accretion in the Universe
    and a precise census of accreting SMBH.

22
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23
MIR selected vs. X-ray selected AGNs
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