Observations of AGN Outflows and Their Contribution to Feedback Gordon Richards Drexel University With thanks to Sarah Gallagher, Karen Leighly, Pat Hall,

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Presentation transcript:

Observations of AGN Outflows and Their Contribution to Feedback Gordon Richards Drexel University With thanks to Sarah Gallagher, Karen Leighly, Pat Hall, Paul Hewett, Nahum Arav, Daniel Proga, TJ Cox, and John Everett

Merger Scenario w/ Feedback merge gas-rich galaxies forms buried AGNs feedback expels the gas reveals the AGN shuts down accretion and star formation Granato et al. 2004, DiMatteo et al. 2005, Springel et al. 2005, Hopkins et al. 2005/6a-z e.g., Silk & Rees 1998, Fabian 1999 Kauffmann & Haehnelt 2000

Why No Big Galaxies? Benson et al Mass Number Expected Observed

Color Mass Color Red Blue Blue Cloud Red Sequence 2 Types of Galaxies e.g., Faber et al. 2007

M BH -sigma From AGN Feedback Di Matteo, Springel, & Hernquist 2005 Simulations of mergers can reproduce this relationship if 5% of the AGN’s radiated luminosity couples with the gas (0.5% of the rest mass enery).

Is Feedback Really Needed? Wuyts et al. 2010, in prep. Still have some post-AGN star formation (still some gas). Would get red ellipicals from merger anyway. Would get red ellipicals from merger anyway. M-sigma may just indicate same fuel source. M-sigma may just indicate same fuel source. AGNs may not make red, dead ellipticals – they just make them better.

Feedback Mechanisms Jets Winds o radiation pressure  line  continuum o magneto-centrifugal forces o thermal pressure Radiative Heating e.g., Begelman 2004

“Quasar” vs. “Radio” Mode Quasar mode = cold gas accretion Quasar mode = cold gas accretion Radio mode = hot gas accretion (Croton et al. 2006) Radio mode = hot gas accretion (Croton et al. 2006) N.B.: AGNs with radio jets aren’t necessarily radio mode objects. I will strictly be talking about quasar mode.

Urry & Padovani 1995 Clouds (and Torus?) => Disk Winds Elvis 2000 Proga 2005 ( see also Everett 2005)

Accretion Disk Radiation (Gallagher et al. 2002a: Adapted from Königl & Kartje 1994; Murray et al. 1995) Black Hole Strong X-rays (~ light hours) Weak X-rays UV Light Optical Light (~ light years)

Accretion Disk Wind Wind (Gallagher et al. 2002a: Adapted from Königl & Kartje 1994; Murray et al. 1995) UV light from the accretion disk pushes on electrons in the “atmosphere” of the accretion disk and drives a wind. This wind deposits energy into the system. Proga et al Dusty region

Broad Absorption Line Quasars Quasars with P-Cygni like absorption troughs reveal much about the nature of the accretion disk wind.Quasars with P-Cygni like absorption troughs reveal much about the nature of the accretion disk wind. Weak X-ray (relative to UV) allows stronger winds.Weak X-ray (relative to UV) allows stronger winds. Hall et al. ‘02; Reichard et al. ‘03a,b; Tolea et al. ‘03; Trump et al. ‘06; Gibson et al. ‘08 P Cygni profile from ejected gas

SED/Shielding Dependence v term ~ (GM BH /R launch ) 1/2 (cf. Chelouche & Netzer 2000; Everett 2005) smaller R launch  higher v term thicker shield  more X-ray weak thinner shield  less X-ray weak larger R launch  lower v term (Gallagher et al. 2006; Gallagher & Everett 2007)

UV Wind Diagnostics Campaigns have concentrated on (Fe)LoBALs. Determine distances, outflow rates, kinetic luminosities. Find typical distance are a few kpc. Outflow rates of tens of solar masses/year. Kinetic luminosities of 0.01 L_bol Crenshaw et al Krolik & Kriss 2001 de Kool et al. 2001; FIRST J Crenshaw, Kraemer, & George 2003; ARAA Moe et al. 2009; SDSS J Bautista et al. 2010; QSO Dunn et al. 2010; SDSS J

SDSS ergs/s = Solar masses/yr Moe et al. 2009

Warm Absorber (X-ray) Examples Turner et al Reynolds et al Blustin et al Chartas et al. 2010, Saez et al (APM ) Chartas et al. 2003, 2007 (PG ) Reeves et al (PDS456) Pounds et al (PG ) Dadina & Cappi 2004 (IRAS ) Zheng & Wang 2008 (CDFS) but see Vaughan & Uttley (2008)

APM (Chartas et al.) Mass outflow rates of 16—64 M_sun/year. Winds are massive and energetic enough to influence galaxy formation (if common). Argue that most of the mass and energy must be carried away by X- ray absorbers Argue that most of the mass and energy must be carried away by X- ray absorbers.

Other X-ray Examples PG ; Chartas et al. 2003/2007 PDS 456; Reeves et al. 2003

The Future?: Winds from Emission We can use 2 key emission line diagnostics from C IV in the redshift range where BALs are found to learn more about winds. These help to identify the parent sample of objects from which BALQSOs are drawn. This will lead to a re-interpretation of the 20% BAL fraction and the realization that strong SED dependences need to be accounted for.

The Baldwin Effect Richards et al More luminous quasars have weaker CIV lines (Baldwin 1977). Seen here from an SDSS sample with 30k quasars.

CIV “Blueshifts” The peak of CIV emission is generally not at the expected laboratory wavelength (e.g., Gaskel 1982). Richards et al. 2010

CIV Parameter Space Radio- Loud BALQSOs Richards et al Can form a joint parameter space with these two observations. Generally speaking radio- loud quasars and BALQSOs live in opposite corners.

2-Component BELR 1.The Disk Dominated by Low-ionization lines Single-peaked due to large distance? 2.The Wind Dominated by High-ionization lines Single-peaked due to radiative transfer effect (Murray & Chiang)

Disk+Wind Leighly 2004

Filtered Continuum In the model of Leighly 2004, the disk isn’t just a separate component, it sees a different continuum than the wind (and possibly different from what we see). Leighly 2004; Leighly & Casebeer 2007

A Range of Intrinsic SEDs Leighly et al While the disk may see a different filtered continuum for different strength winds, the structure of the wind depends on the intrinsic SED.

More ionizing flux = strong disk component High radio-loud prob; low BALQSO prob Less ionizing flux = strong wind component Low radio-loud prob; high BALQSO prob

CIV Parameter Space Radio- Loud BALQSOs Richards et al Ionizing SED, Weak LD winds Less ionizing SED, Strong LD winds SEDs affects winds, which affects covering fractions. Mass and accretion rate affect SEDs (i.e., the SEDs evolve). 40% 0%

Conclusions However, we must realize that ALL QUASARS ARE NOT THE SAME! We need to get away from the nearly religious adherence to: The Unified Model A Universal SED A 20% BAL fraction Evolution vs. Orientation There’s plenty of evidence for winds in AGNs and that they can cause feedback effects.