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The Evolution of The Evolution of AGN Obscuration AGN Obscuration Ezequiel Treister Ezequiel Treister (ESO) (ESO) Meg Urry (Yale) Julian Krolik (JHU)

The Evolution of AGN Obscuration

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The Evolution of AGN Obscuration. Ezequiel Treister (ESO) Meg Urry (Yale) Julian Krolik (JHU). Supermassive Black Holes. Many obscured by gas and dust. How do we know that? Local AGN Unification Explain Extragalactic X-ray “Background”. - PowerPoint PPT Presentation

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Page 1: The Evolution of AGN Obscuration

The Evolution of The Evolution of AGN ObscurationAGN Obscuration

Ezequiel Treister (ESO)Ezequiel Treister (ESO)

Meg Urry (Yale)

Julian Krolik (JHU)

Page 2: The Evolution of AGN Obscuration

Supermassive Black Supermassive Black Holes Holes

Credit: ESO/NASA, the AVO project and Paolo Padovani

Many obscured by gas and dustMany obscured by gas and dust

How do we know that?How do we know that?

Local AGN Unification

Explain Extragalactic X-ray “Background”

Page 3: The Evolution of AGN Obscuration

Observed X-ray Observed X-ray “Background”“Background”

Frontera et al. (2006)

Page 4: The Evolution of AGN Obscuration

X-ray BackgroundX-ray Background

Treister & Urry, 2005

XRB well explained using a combination of obscured and unobscured AGN.

•Setti & Woltjer 1989•Madau et al. 1994•Comastri et al. 1995•Gilli et al. 1999,2001•And others…

Page 5: The Evolution of AGN Obscuration

Obscured AGN FractionObscured AGN Fraction

Treister & Urry (2005) Observational data from

Barger et al. (2005)

Page 6: The Evolution of AGN Obscuration

Obscured AGN FractionObscured AGN Fraction

Treister & Urry (2005) Observational data from

Barger et al. (2005)

Page 7: The Evolution of AGN Obscuration

Obscured AGN FractionObscured AGN Fraction

Treister & Urry (2005) Observational data from

Barger et al. (2005)

Page 8: The Evolution of AGN Obscuration

Redshift Dependence?Redshift Dependence?

Treister & Urry (2005) Observational data from

Barger et al. (2005)

Incompleteness doesnot allow to rule-out intrinsically constant fraction of obscured AGN.

Page 9: The Evolution of AGN Obscuration

Meta-SurveyMeta-Survey

• 7 Surveys, • 2341 AGN, 1229 w Ids• 631 Obscured (no broad lines)• 1042<Lx<1046, 0<z<5

Treister & Urry, 2006

Page 10: The Evolution of AGN Obscuration

Bivariate X-ray and optical flux Bivariate X-ray and optical flux limitslimits

Treister & Urry, 2006

Spectroscopic incompleteness is a strong function of optical magnitude.

Page 11: The Evolution of AGN Obscuration

Total effective area of meta-Total effective area of meta-surveysurvey

Treister & Urry, 2006

Page 12: The Evolution of AGN Obscuration

Ratio vs RedshiftRatio vs Redshift

Treister & Urry, 2006

Page 13: The Evolution of AGN Obscuration

Ratio vs RedshiftRatio vs Redshift

Treister & Urry, 2006

Page 14: The Evolution of AGN Obscuration

Ratio vs RedshiftRatio vs Redshift

Treister & Urry, 2006

Evolution independentof choice of hostGalaxy (only reallyImportant parameter).

See Also:La Franca et al. 2005Ballantyne et al. 2006Akylas et al. 2006

Page 15: The Evolution of AGN Obscuration

Ratio vs LuminosityRatio vs Luminosity

Treister & Urry, 2006

Page 16: The Evolution of AGN Obscuration

A Changing Torus?A Changing Torus?A change in the IR/NUV flux ratio may indicate a change in torus geometry.

~2x

Granato & DaneseTorus model

Page 17: The Evolution of AGN Obscuration

A Changing Torus?A Changing Torus?SampleSample

Completely unobscured AGNNarrow redshift range, 0.8<z<1.2Wide range in luminosityData at 24 µm from Spitzer

High LHigh L•SDSS DR5 Quasar sample•11938 quasars, 0.8<z<1.2•192 with Spitzer 24 µm photometry•157 of them with GALEX UV data

Low LLow L•GOODS: North+South fields•10 unobscured AGN•All with Spitzer 24 µm photometry•8 with GALEX UV data

Page 18: The Evolution of AGN Obscuration

A Changing Torus?A Changing Torus?Bolometric luminosityconstructed from NUVto mid-IR.

No change in NUV/Bolratio with luminosity!

Treister & Krolik, in prep.

Page 19: The Evolution of AGN Obscuration

A Changing Torus?A Changing Torus?

Change in 24 µm/Bolratio with luminosity!

Lower ratio at high L Consistent with larger opening anglesat higher luminosities.

Treister & Krolik, in prep.

Page 20: The Evolution of AGN Obscuration

Compton Thick AGNCompton Thick AGN

Defined as obscured sources with NH>1024 cm-2.

Very hard to find (even in X-rays). Observed locally and needed to

explain the X-ray background. Number density highly uncertain. High energy (E>10 keV)

observations are required to find them.

Page 21: The Evolution of AGN Obscuration

INTEGRAL AGN logN-logSINTEGRAL AGN logN-logS

Treister et al, submitted

Data points from Beckmann et al. 2006

Page 22: The Evolution of AGN Obscuration

Space Density of CT AGNSpace Density of CT AGN

Treister et al, submitted

CT AGN Factor, ~0.25

Page 23: The Evolution of AGN Obscuration

XRB IntensityXRB Intensity

Page 24: The Evolution of AGN Obscuration

X-ray BackgroundX-ray Background

Gilli et al, 2006

• Spread in • Original XRB normalizationStrong degeneracy between XRB intensity and density of CT AGN

Page 25: The Evolution of AGN Obscuration

Compton Reflection Compton Reflection ComponentComponent

Treister et al, submitted

XRB IntensityHEAO-1 OriginalINTEGRALHEAO-1 +40%

Treister & Urry, 2005

CT AGN Space Density

High Ref. Component, ~2.Not observed on individual AGN

Most likely solution.Gilli et al. 2006

Page 26: The Evolution of AGN Obscuration

SummarySummaryThe obscured AGN fraction decreases with

increasing luminosity. Ratio of IR to Bolometric luminosity in

unobscured AGN suggest this is due to a change in opening angle.

The obscured AGN fraction increases with redshift as (1+z)0.4.

Observed spatial density of CT AGN and individual sources favors the original HEAO-1 XRB intensity with a Compton reflection component of ~1.

Page 27: The Evolution of AGN Obscuration
Page 28: The Evolution of AGN Obscuration

u-z SDSS QSO Colorsu-z SDSS QSO Colors