Extragalactic X-ray Surveys: Source Populations and their Evolution. Paul Green SAO

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Transcription:

Extragalactic X-ray Surveys: Source Populations and their Evolution Paul Green SAO X-ray School 2011

I ll speak only about serendipitous, extragalactic X-ray surveys from focusing telescopes, and almost exclusively about AGN and Galaxies Preface This review, like so many surveys, will be - incomplete - biased Survey types include SYNOPTIC - repeated monitoring KNOWN OBJECTS - pointed sample surveys - raster/mosaic/tiling of individual objects SERENDIPITOUS - deep pencil beam serendipitous - raster/ mosaic/ tiling of blank sky region - all-sky serendipitous

Dangers of Targeted Samples Kennicut 1990 X-ray School 2011

Dangers of Targeted Samples Kennicut 1990 X-ray School 2011

Outline Why survey? Advantages and characteristics of X-ray selection Historical X-ray surveys The logn-logs Cosmic X-ray Background Current surveys, Deep and Wide Analyzing survey data Multiwavelength followup Source types Science Motivations Science Results

Why Survey? Census of the Universe Outliers, novel sources and serendipity. Resolve the Cosmic X-ray background. Accumulate a statistical samples. Study populations, e.g. Luminosity functions Spectral energy distributions Accretion, star formation Clustering Morphology Evolution X-ray School 2011

X-ray Survey Advantages Most X-ray sources are AGN (purity). Most AGN produce X-rays (completeness). Surface density of X-ray-selected AGN far exceeds optical AGN by 10-20 (Bauer et al 2004) X-rays sample the circumnuclear region (R<100*R grav ) Weaker z-dependence than optical. X-rays penetrate large columns of gas and dust. Negative k-correction favors high-z N eff H ~Nintr H / (1+z)2.6

Striking how modest the number of X-ray sources is compared to the number of optical sources X-ray School 2011

Advantage: Penetrating Power of X-rays

Advantage: High contrast between AGN and stellar light

Advantage: High contrast between AGN and stellar light

X-ray Survey Downers X-ray detectors are non-uniform PSF size and flux sensitivity vary with off-axis angle Deep or wide X-ray surveys are expensive & time consuming Cosmic Variance can use serendipitous detections from archived observations Require multi-wavelength followup and usually spectroscopy

Early X-ray Surveys Uhuru (1970-1973) [2-20 kev] Ariel-V (1973-1980) [0.3-40 kev] HEAO-1 (1977-1979) [0.2keV-10MeV]

Soft X-ray Surveys Einstein (1978-1981) [0.2-20 kev] aka HEAO-2, first imaging telescope ROSAT (1990-1999) [0.1-2.5 kev]

Hard X-ray Surveys ASCA (1993-2001 ) [0.4-10 kev] BeppoSAX (1996-2002) [0.1-300 kev] INTEGRAL/IBIS (2002 - ) [15keV - 10 MeV] Swift/BAT (2004 - ) [15-150 kev]

The Hard X-ray Sky: Mostly AGN ADAPTED FROM SWIFT- BAT/ INTEGRAL- IBIS SURVEYS (CUSUMANO ET AL. 2010, BIRD ET AL. 2010, TUELLER ET AL. 2009, KRIVONOS ET AL. 2007) X-ray School 2011 (Credit F. Panessa 2011)

Most X-ray Sources are AGN Variability Soldi et al. 2008 X-ray School 2011

Chandra and XMM-Newton Surveys Chandra (1999-present) XMM-Newton (1999-present)

Just Count the Sources: the logn-logs Derive the source density on the sky as a function of flux. Requires detailed understanding of survey sensitivity and area. Given an assumed cosmology, the logn-logs places limits on source populations, luminosity functions, and evolution. Population models must eventually reproduce the lognlogs, including how it changes with observed bandpass. X-ray School 2011

The Extragalactic log-n-logs = ρv = ρ

Flux Limits Flux limit is a function of Telescope effective area and Exposure Background level (particle, diffuse bkg, and unresolved/undetected sources) PSF (function of detector position) Source spectrum Definitions of f X lim differ: Counts flux S/N Prob % Completeness X-ray School 2011

ChaMP X-ray Simulations SAOSAC raytrace simulations Grid of off-axis angles 10 1000 count sources Std XPIPE detection & Photometry Compare input/output - detection rates - positions

X-ray Sensitivity & Incompleteness Detailed corrections required for an accurate logn-logs or XLF using full field area: Total survey area vs. flux Limiting flux at each pixel Incompleteness

ChaMP logn-logs Kim et al. 2004 Soft Band Hard Band Bridges flux gaps between ROSAT, ASCA & Chandra Deep Fields Results consistent with CDFs and XMM

ChaMP logn-logs: Results Kim et al. 2004 Soft band differential logn-logs requires a broken powerlaw β bright =2.3±0.2, β faint =1.7±0.1, S break =6 10-15 Hard band: β=1.3±0.1 single PL acceptable Results consistent with XMM (Baldi et al. 2001) CDF-N (Brandt et al. 2001)

The Cosmic X-ray Background and AGN Population Synthesis Chandra bandpass Comastri et al. 1995 Discovered 1962 (Giacconi et al., flying Geiger counters) Peaks at ~30keV Not hot gas, since expected CMB distortion s not seen (Wright et al. 1994)

The Formerly Diffuse Cosmic X-ray Background (Moretti et al. 2003) About 80% of the 2-8 kev CXRB resolved: CDF-N (Brandt et al. 02), CDF-S (Giacconi et al 01), Lockman Hole (Hasinger et al. 01)

Most of the Rest Associated with Faint Galaxies Hickox & Markevitch 2007 after excluding Chandra, HST and Spitzer IRAC sources, only only a marginal % of Chandra CXB still remains X-ray School 2011

The Unresolved Hard X-ray Background (XMM and Chandra Deep Fields) Total CXRB emission point source contributions N H =4.5e23 @ z=0.8 (Worsley et al. 2005)

The CXRB and AGN Population Synthesis Ballantyne et al. 2011 XRB Data: Beppo-SAX ASCA/SIS ASCA/GIS XMM XMM RXTE Data Points: Swift/XRT Swift/BAT INTEGRAL INTEGRAL HEAO-1 5 recent AGN evolution models (solid lines) and their Compton thick components (dashed). Model parameters include HXLF, Γ dispersion, reflection efficiency, CT ratio, and evolution.

Deep Extragalactic X-ray Surveys (>75ksec) Brandt 2005 ARAA ADD: C-COSMOS 1.8Ms; CDFS 3.8Ms

Chandra Advances ~1 positions, small PSF & low background 10-100 fainter flux limits unambiguous source IDs Source extent and morphology XMM-Newton is Complementary 4 Effective Area + larger Field-of-View Harder energy band: 0.5-20 kev

Chandra Extragalactic Surveys Deeper Hickox et al. 2009 Wider

Chandra Deep Field South CDF-S: 4Msec in 52 obsids, May 2000 - July 2010. Merged dataset at http://cxc.harvard.edu/cda/contrib/cdfs.html GOODS-S UDF UDF Greyscale image: 26 x 26 False color image: Central 8 x 8

Source Matching Ambiguity Image: R <~ 27mag X-ray contours: logarithmic 0.003% to 30% of max Fraction of matched / multiple/ spurious all depend on PSF size, and relative flux limits Demands visual inspection Xue et al. 2011 X-ray School 2011

Deep Extragalactic X-ray Surveys Source classification difficulties Many of the X-ray sources have modest optical luminosities, often due to obscuration Many are too faint to be identified by optical spectra AGN unification is broken between optical (type1 and type2) and X-ray (unobscured and obscured )

ChaMP Optical Spectroscopic Program J. Silverman, P. Green, P. Smith, E. Romero-Colmenero (SAAO), A. Constantin, M. Trichas Spectroscopic identification r <22 nd mag 24 Fields 445 IDs 52% BLAGN Broad emission Line AGN (FWHM > 1000 km/s) 25% NELG Narrow Emission Line Galaxy (FWHM<1000 km/s; W e λ >5 Å) 11% ALG (absorption line galaxy) 13% Stars 1% Clusters

Basic AGN Types from X-ray Surveys Unobscured AGN Obscured AGN with clear optical/uv AGN signatures. Optically faint X-ray sources XBONGs

Basic AGN Types from X-ray Surveys Unobscured AGN Obscured AGN with clear optical/uv AGN signatures. Optically faint X-ray sources XBONGs (X-ray Bright Optically Normal Galaxies)

Wide Extragalactic X-ray Surveys Amass rare bright sources Smooth out cosmic variance. Bridge flux gap between deep and all-sky surveys Still sufficiently deep that complete source classification is quite challenging X-ray School 2011

Wide Extragalactic X-ray Surveys Chandr ChaMP a (Green et al. 2004; Kim et al 2004) CYDER (Treister 2005) CLASXS (Lockman Hole; Steffen, Barger, Yang) XBootes/NDWFS (Murray, Jones, Kenter, Brand) SEXSI (Harrison, Helfand) XMM-Newton HELLAS2XMM (Baldi, Fiore, Brusa) XMM/2dF (Georgakakis, Georgantopolous) XMM-SSC (Watson) XMM-LSS (Pierre) X-ray School 2011

Combining Deep & Wide for XLFs Silverman et al. 2008 Survey area vs fx limit r mag Completeness map L, z bins for XLF log f X (2-8keV) X-ray School 2011

X-ray Luminosity Function (2-8 kev) 1/V a method Identified fraction 0.3 < C(i) < 1.0 Ω M =0.3, Ω Λ =0.7, H o =70 km s -1 Mpc -1

What We Think We Know Relevant to SMBHs and their Evolution ΛCDM Cosmology & Hierarchical Structure Formation Luminous quasars peaked at z=2 SMBHs are common in local galaxies The CXRB is resolved at low energies and may be explained by absorbed AGN

The Quasar Epoch Silverman et al. 2005 X-ray School 2011

Downsizing Brightest QSOs peak at z~2.5 (or higher). Faintest QSOs peak at z~1 (or lower). Croom et al. 2008 X-ray School 2011

M BH -σ Relation Correlation between SMBH mass and mass of the galaxy spheroid (via velocity dispersion σ V ) M BH (M ) Gültekin et al. 2009 AGN and star formation activity may be concurrent AGN play key role in galaxy formation and evolution σ (km/s) X-ray School 2011

AGN Fueling in a Gas-Rich Major Merger (c) Interaction/ Merger (d) Coalescence/ (U)LIRG (e) Blowout (f) Quasar (b) Small Group (a) Isolated Disk L QSO SFR (g) Decay/K+A (h) Dead Elliptical Hopkins et al. 2008 Time (Relative to Merger) X-ray School 2011

AGN/Host Co-Evolution Cartoon Here luminous accretion occurs preferentially where M halo~ ~10 12-10 13 M sun Hickox (2009) X-ray School 2011

What We Know We Don t Know - What objects constitute the CXRB? - What fraction of AGN are obscured? As a function of L. Of z. - Do obscured and unobscured populations evolve in the same manner? - How much SMBH accretion is hidden from optical/x-ray/ir surveys? - What modes of accretion are there? What are their hosts? Their environments? - How much and when do accretion and star formation overlap? - Are local quiescent SMBHs relics of the bright quasars?

ChaMP + SDSS Chandra ACIS- S Chandra ACIS-I SDSS DR5 Covey et al. 2008 392 Chandra Cycle 1-6 ACIS Fields: ~33 deg 2 Exposures: 1-120 ks (median = 21 ks, total = 8.4 Ms) X-ray detections or limits for all SDSS sources in ChaMP area X-ray School 2011

Active Fraction Sub-Samples Divide sample into 5 volume-limited optical samples Calculate fraction for any L X threshold Haggard et al. 2010 M i M i log L x = 42 0.0 0.2 0.4 0.6 0.8 bestz log L x

AGN Fraction by Redshift, M i and Host Galaxy Stellar Mass Trend with bestz tracks AGN/QSO X-ray LF Stronger trends with M i and Mass Haggard et al. 2010 AGN Fraction (%) XLF ~ (1+z) 3 bestz M i log M * (M ) X-ray School 2011

Comparing Field & Cluster Fractions Excellent agreement w/ Martini et al. (2007) cluster fractions: clusters 0.05 < z < 0.31, 35 X-ray-detected (M R < -20) galaxies At low-z, apparent X-ray point source overdensities toward clusters simply track cluster galaxy overdensity M R < logl x N x N opt Frac Err Cluster min max % % -20 40.9 43.6 28 476 6.0 1.1 6.0-20 41.0 30 663 4.5 0.8 4.9-20 42.0 110 9415 1.2 0.1 1.0-21.3 41.0 27 232 12.4 2.3 9.8 X-ray School 2011

Field vs. Cluster Fraction Mergers may not be fueling AGN in the local Universe? Other fueling mechanisms at work? OR a conspiracy where Other fueling mechanisms more efficient in clusters Major mergers still prevail in the field Morphological evidence in the field shows no merger excess among 0.3<z<1 AGN (COSMOS; Cisternas et al. 2010) X-ray School 2011

AGN Fraction by Host Color Color is a proxy for morphology Does F AGN peak in the green valley, blue cloud or the red sequence? May shed light on dominant fueling mechanism (u-r) 0 Red: (u-r) 0 0.6 Green: 1.8 < (u-r) 0 < 2.6 Blue: (u-r) 0 2.6 M i X-ray School 2011

Active Fraction by Restframe (u-r) 0 Color Larger fractions in the Blue Cloud for all L x Cumulative X-ray-active Fraction [%] sample 4-22 > M i > -23 z 0.55 log Lx (0.5-2.0 kev) erg s -1 X-ray School 2011

Conclusions X-ray survey sensitivity and completeness should be well-characterized. Multiwavelength observations are crucial. Matching to counterparts should be careful. Spectroscopic completeness also crucial. OK, so it ain t easy! AGN/galaxy/structure co-evolution is a new and exciting frontier in astrophysics. Successful models should match CXRB logn-logs XLFs current local SMBH mass function host galaxy properties environments and clustering evolution X-ray School 2011

The End

XBootes 126*5ksec Raster X-ray School 2011