The Impact of 'Quasar' Feedback on the Formation - TAPIR Group at ...
The Impact of 'Quasar' Feedback on the Formation - TAPIR Group at ...
The Impact of 'Quasar' Feedback on the Formation - TAPIR Group at ...
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<str<strong>on</strong>g>The</str<strong>on</strong>g> <str<strong>on</strong>g>Impact</str<strong>on</strong>g> <str<strong>on</strong>g>of</str<strong>on</strong>g> “Quasar”<br />
<str<strong>on</strong>g>Feedback</str<strong>on</strong>g> <strong>on</strong> <strong>the</strong> Form<strong>at</strong>i<strong>on</strong> &<br />
Evoluti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> Red Galaxies<br />
Philip Hopkins 07/17/06<br />
Lars Hernquist, Volker Springel, Gord<strong>on</strong> Richards, T. J. Cox,<br />
Brant Roberts<strong>on</strong>, Tiziana Di M<strong>at</strong>teo, Yuexing Li, Sukanya Chakrabarti
Motiv<strong>at</strong>i<strong>on</strong><br />
Tremaine+ 02; Onken+ 04; Nels<strong>on</strong>+ 04;<br />
Peters<strong>on</strong>+ 04, 05; Barth+ 04, 05;<br />
Greene & Ho 05<br />
Baldry+ 04<br />
u-r<br />
Bell+ 04
A General Framework...<br />
galaxy<br />
mergers<br />
hierarchical<br />
growth<br />
normal galaxies<br />
(dead quasars)<br />
gas<br />
inflows<br />
galaxy form<strong>at</strong>i<strong>on</strong><br />
and evoluti<strong>on</strong><br />
AGN<br />
feedback<br />
starbursts &<br />
buried quasars<br />
growth <str<strong>on</strong>g>of</str<strong>on</strong>g><br />
supermassive black holes<br />
active<br />
quasars
<str<strong>on</strong>g>The</str<strong>on</strong>g> Semi-Analytic Approach<br />
Galaxy<br />
“<str<strong>on</strong>g>Feedback</str<strong>on</strong>g>”<br />
Galaxy<br />
Galaxy<br />
NGC 6240 (Keel 1990)
Real Systems Are Messy!<br />
HUGE RANGE OF COMPLEX & UNCERTAIN PHYSICS<br />
<br />
Need to tre<strong>at</strong>:<br />
Orbits+torquing (3-D)<br />
Star form<strong>at</strong>i<strong>on</strong><br />
Cooling<br />
SNe <str<strong>on</strong>g>Feedback</str<strong>on</strong>g><br />
BH <str<strong>on</strong>g>Feedback</str<strong>on</strong>g><br />
Metal Enrichment<br />
Shocks<br />
Huge range <str<strong>on</strong>g>of</str<strong>on</strong>g> initial c<strong>on</strong>diti<strong>on</strong>s
How to Model <str<strong>on</strong>g>The</str<strong>on</strong>g>se Processes?<br />
(HOW TO GET THE BEST BANG FOR YOUR SUPERCOMPUTING BUCK)<br />
<br />
Ideally, would use cosmological simul<strong>at</strong>i<strong>on</strong>s:<br />
Millenium run resoluti<strong>on</strong> ~ 5 h^-1 kpc<br />
<br />
<br />
Adaptive mesh “zoom-in” runs similarly too expensive<br />
Wh<strong>at</strong> if <strong>the</strong> cosmological simul<strong>at</strong>i<strong>on</strong> doesn’t make disks?
E1)/#412%#HI")&6*.'(#,)%J.2"#+1($4"-#(%#KC!#412%L<br />
!<br />
!"#$%+,*("#(4"#"31$(#0)1M.(1(.%&12#,%<br />
<str<strong>on</strong>g>The</str<strong>on</strong>g> Simul<strong>at</strong>i<strong>on</strong>s 8("221)#-.'/#H"3,%&(.12L<br />
J%)#(4"#13.'5++"().$#+1''#-.'().7*(.%&<br />
8("221)#7*20"<br />
'%2M"#(4"#N"1&'#"6*1(.%&'<br />
INSTEAD, MODEL INDIVIDUAL GALAXY MERGERS AT HIGH RESOLUTION<br />
!<br />
F1'#,)"''*)"#"JJ"$('#1)"#.&$2*-"-<br />
F1'"%*'#-.'/#H"3,%&(.12L<br />
!<br />
94"#01'"%*'#'$12"O4".04(#.'#122%P"-#(%<br />
<str<strong>on</strong>g>The</str<strong>on</strong>g> Simul<strong>at</strong>i<strong>on</strong>s<br />
STILL, CAN’T RESOLVE EVERYTHING...<br />
<br />
Individual sites <str<strong>on</strong>g>of</str<strong>on</strong>g> star form<strong>at</strong>i<strong>on</strong> still > “sink” <str<strong>on</strong>g>of</str<strong>on</strong>g> molecular clouds >> star form<strong>at</strong>i<strong>on</strong> >> SNe feedback<br />
pressurizes hot phase & evapor<strong>at</strong>es clouds<br />
Kennicutt ‘98<br />
Simul<strong>at</strong>i<strong>on</strong>s
<str<strong>on</strong>g>The</str<strong>on</strong>g> Simul<strong>at</strong>i<strong>on</strong>s<br />
THE AGN...<br />
R_sch ~ few AU ~<br />
10^-6 x our resoluti<strong>on</strong><br />
<br />
R_B<strong>on</strong>di ~ 10 pc (typical)<br />
<br />
<br />
<br />
B<strong>on</strong>di-Hoyle accreti<strong>on</strong> r<strong>at</strong>e<br />
(max Eddingt<strong>on</strong>)<br />
~0.1 radi<strong>at</strong>ive efficiency<br />
(high-mdot)<br />
~5% couples to local gas<br />
(<strong>the</strong>rmally)
<str<strong>on</strong>g>The</str<strong>on</strong>g> Simul<strong>at</strong>i<strong>on</strong>s<br />
A CAUTION...<br />
Pellegrini ‘05<br />
#$"#%&'(&)*%+&$,-,.*"%&/#*$$"#&%/,#01#/%&,2)&*$2*/"&3"2/#,-&456&,3/*7*/8<br />
90+% <str<strong>on</strong>g>of</str<strong>on</strong>g> feedback<br />
;&;?9:=6&=@&A94B&@=B!49:=6&B49;&46C&D>4EF&G=>;&5B=H9G&:6&4&!;B5;B<br />
!"#$"#%&'%()*$"*"++%,-+.+<br />
!"#$"#%&'%,-+.+%/-01%()*$"+<br />
DG&I,%%<br />
DG&I,%%<br />
DG&,33#"/*'2&#,/"<br />
JKL&<br />
;))*2$/'2&<br />
#,/"<br />
DG&,33#"/*'2&#,/"<br />
<br />
But, feedback effects not sensitive<br />
to <strong>the</strong> accreti<strong>on</strong> prescripti<strong>on</strong>!
<str<strong>on</strong>g>The</str<strong>on</strong>g> Simul<strong>at</strong>i<strong>on</strong>s<br />
INITIAL, IMPULSIVE FEEDBACK VS. “MAINTENANCE”<br />
We see today...<br />
but...<br />
White+ 06<br />
Ho 02<br />
<br />
Even with low (
<str<strong>on</strong>g>The</str<strong>on</strong>g> Simul<strong>at</strong>i<strong>on</strong>s<br />
WHAT ABOUT THE FEEDBACK PRESCRIPTION?<br />
<br />
Modeling “Quasar” <str<strong>on</strong>g>Feedback</str<strong>on</strong>g><br />
~5% to m<strong>at</strong>ch observed M-sigma normaliz<strong>at</strong>i<strong>on</strong> (Silk & Rees ‘98)<br />
<br />
<br />
<br />
<br />
Line opacities + AGN spectrum (Saz<strong>on</strong>ov et al.)<br />
Momentum driven winds (Murray et al.)<br />
Disk wind simul<strong>at</strong>i<strong>on</strong>s (Proga et al.)<br />
<br />
Probably not radio jets
<str<strong>on</strong>g>The</str<strong>on</strong>g> Simul<strong>at</strong>i<strong>on</strong>s<br />
FINALLY, WHAT TO SIMULATE?<br />
<br />
Span <strong>the</strong> parameter space, varying:<br />
<br />
<br />
<br />
<br />
<br />
<br />
<br />
<br />
Masses & mass r<strong>at</strong>ios<br />
Disk gas fracti<strong>on</strong>s<br />
Redshift <str<strong>on</strong>g>of</str<strong>on</strong>g> form<strong>at</strong>i<strong>on</strong> & merger<br />
Disk structural parameters<br />
<br />
Bulge-to-disk r<strong>at</strong>io,<br />
c<strong>on</strong>centr<strong>at</strong>i<strong>on</strong>, scale lengths<br />
ISM <str<strong>on</strong>g>Feedback</str<strong>on</strong>g>/Pressuriz<strong>at</strong>i<strong>on</strong><br />
(iso<strong>the</strong>rmal > full multiphase)<br />
BH accreti<strong>on</strong> & feedback efficiency<br />
Stellar winds : add/remove<br />
<br />
Mass loading, energy-loading<br />
Orbital parameters<br />
<br />
<br />
<br />
Disk orient<strong>at</strong>i<strong>on</strong>s<br />
Angular momentum<br />
Pericentric passage<br />
~500+ simul<strong>at</strong>i<strong>on</strong>s and counting (Roberts<strong>on</strong> et al. 2005; Cox et al. 2004)
Quasar Growth:<br />
GAS IS HEATED AND EXPELLED IN BLOWOUT, REVEALING A BRIEF, BRIGHT QUASAR<br />
Bahcall 96<br />
NGC 6240 (Keel 1990)<br />
Column Densities<br />
Bolometric<br />
“Blowout”<br />
phase<br />
B-Band<br />
Luminosity
<str<strong>on</strong>g>Feedback</str<strong>on</strong>g>-driven “Blowout” Gives M-sigma Rel<strong>at</strong>i<strong>on</strong><br />
PREVENTS RUNAWAY BLACK HOLE GROWTH<br />
Di M<strong>at</strong>teo et al. 2005<br />
Black hole growth<br />
without feedback<br />
with feedback<br />
(Gebhardt et al. 2000;<br />
Ferrarese & Merritt 2000;<br />
Tremaine et al. 2002)<br />
Springel et al. 2004
Expulsi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> Gas Turns <str<strong>on</strong>g>of</str<strong>on</strong>g>f Star Form<strong>at</strong>i<strong>on</strong><br />
ENSURES ELLIPTICALS ARE SUFFICIENTLY “RED & DEAD”<br />
Springel et al. 2005<br />
No AGN<br />
<str<strong>on</strong>g>Feedback</str<strong>on</strong>g><br />
With AGN<br />
<str<strong>on</strong>g>Feedback</str<strong>on</strong>g>
Every Quasar Has a Host<br />
MAPPING BETWEEN MERGER DISTRIBUTIONS<br />
galaxy<br />
mergers<br />
hierarchical<br />
growth<br />
normal galaxies<br />
(dead quasars)<br />
Spheroids + QSOs produced<br />
toge<strong>the</strong>r<br />
<br />
Hosts follow M-sigma (Di M<strong>at</strong>teo et al.), BH-bulge<br />
mass, Fundamental Plane (Roberts<strong>on</strong> et al.),<br />
Kinem<strong>at</strong>ic/Morphological/Gas Properties (Cox et al.)<br />
Map each quasar to a spheroid<br />
gas<br />
inflows<br />
starbursts &<br />
buried quasars<br />
galaxy form<strong>at</strong>i<strong>on</strong><br />
and evoluti<strong>on</strong><br />
growth <str<strong>on</strong>g>of</str<strong>on</strong>g><br />
supermassive black holes<br />
active<br />
quasars<br />
AGN<br />
feedback<br />
e.g. red galaxy mass functi<strong>on</strong> (dry mergers a small effect)<br />
Bell+<br />
Hopkins et al. 2006c
Every Quasar Has a Host<br />
MAPPING BETWEEN MERGER DISTRIBUTIONS<br />
<br />
Comparing with joint<br />
LFs (NUV,U,B,V,R,I,K)<br />
suggests reliable<br />
empirical model <str<strong>on</strong>g>of</str<strong>on</strong>g><br />
popul<strong>at</strong>i<strong>on</strong> buildup<br />
Hopkins et al. 2006c<br />
Bell+,Willott+,Faber+,<br />
Madgwick+,Giall<strong>on</strong>go+
<str<strong>on</strong>g>The</str<strong>on</strong>g> Color-Magnitude Diagram<br />
Full Model<br />
<br />
More than <strong>on</strong>e effect here!<br />
Hopkins et al. 2006c (obs: Bell+; Faber+)
Multiple Age Measurements to Use as Checks<br />
Jorgensen+; Kels<strong>on</strong>+; Van der Wel+; Holden+; Van Dokkum+; Wuyts+<br />
Age-sigma<br />
Shen+; Trujillo+; McIntosh+<br />
M/L R<strong>at</strong>ios<br />
Size-Luminosity<br />
Rel<strong>at</strong>i<strong>on</strong><br />
Hopkins et al. 2006c
Driving <strong>the</strong> Blue-Red Transiti<strong>on</strong>?<br />
DIRECT OBSERVATIONS<br />
Sanchez+ ‘05<br />
GEMS<br />
0.5 < z < 1.1<br />
Optical QSOs<br />
(also, Kauffmann+ 03;<br />
local SDSS hosts)<br />
Nandra+ ‘06<br />
DEEP2<br />
0.7 < z < 1.4<br />
X-ray QSOs<br />
<br />
Testing *how* color &<br />
accreti<strong>on</strong> r<strong>at</strong>e co-evolve<br />
can break model<br />
degeneracies
<str<strong>on</strong>g>Feedback</str<strong>on</strong>g>-Driven Winds<br />
GENERAL PROPERTIES<br />
<br />
<br />
<br />
Rapid growth (t_S
<str<strong>on</strong>g>Feedback</str<strong>on</strong>g>-Driven Winds<br />
COMPARISON TO STARBURST-DRIVEN WINDS<br />
Mass Loading<br />
Energy Loading<br />
<br />
<br />
<br />
Wind Structure Similar<br />
Different Scales<br />
Different Efficiencies
<str<strong>on</strong>g>Feedback</str<strong>on</strong>g>-Driven Winds<br />
COMPARISON TO STARBURST-DRIVEN WINDS
<str<strong>on</strong>g>Feedback</str<strong>on</strong>g>-Driven Winds<br />
COMPARISON TO STARBURST-DRIVEN WINDS
<str<strong>on</strong>g>Feedback</str<strong>on</strong>g>-Driven Winds<br />
METAL ENRICHMENT<br />
BH<br />
no BH
<str<strong>on</strong>g>Feedback</str<strong>on</strong>g>-Driven Winds<br />
METAL ENRICHMENT & BUILDING THE X-RAY HALO<br />
BH<br />
no BH<br />
Cox et al. 2005
<str<strong>on</strong>g>Feedback</str<strong>on</strong>g>-Driven Winds<br />
HEATING & ENTROPY<br />
<br />
Single, high-impact event can “set up” observed<br />
T/S pr<str<strong>on</strong>g>of</str<strong>on</strong>g>iles & correl<strong>at</strong>i<strong>on</strong>s in ellipticals<br />
<strong>Group</strong>s, even Clusters as well?<br />
BH<br />
no BH
<str<strong>on</strong>g>Feedback</str<strong>on</strong>g>-Driven Winds<br />
HEATING & ENTROPY<br />
<br />
Single episode he<strong>at</strong>s enough gas to<br />
prevent a doubling <str<strong>on</strong>g>of</str<strong>on</strong>g> galaxy size:<br />
<br />
Soluti<strong>on</strong> to cooling flows? Probably not, but<br />
supplements “radio mode”
Observ<strong>at</strong>i<strong>on</strong>al Prospects<br />
“QUASAR” WINDS<br />
<br />
<br />
<br />
High-velocity outflows<br />
>~ 1000 km/s <strong>at</strong> 1-1000 kpc<br />
Local metal absorbers (Bowen+ 06)<br />
BALs <strong>at</strong> “large distances” (deKool+ 01)<br />
High-v outflow in n<strong>on</strong>-BALs (Pounds 06)<br />
Clumpy substructure<br />
Preferentially w. high-Eddingt<strong>on</strong> r<strong>at</strong>io?
Observ<strong>at</strong>i<strong>on</strong>al Prospects<br />
“QUASAR” WINDS<br />
CO outflows (Narayanan et al. 06)
Observ<strong>at</strong>i<strong>on</strong>al Prospects<br />
INDIRECT EFFECTS<br />
Blue - Red transiti<strong>on</strong> :<br />
colors/age <str<strong>on</strong>g>of</str<strong>on</strong>g> SB vs. Mdot<br />
Metal Enrichment<br />
Abundance r<strong>at</strong>ios (where/when are <strong>the</strong> metals from?)<br />
Compare high-z merger pr<str<strong>on</strong>g>of</str<strong>on</strong>g>iles to local spheroids
Summary<br />
A number <str<strong>on</strong>g>of</str<strong>on</strong>g> lines <str<strong>on</strong>g>of</str<strong>on</strong>g> evidence argue for some<br />
form <str<strong>on</strong>g>of</str<strong>on</strong>g> “quasar” feedback<br />
<br />
But need observ<strong>at</strong>i<strong>on</strong>s to<br />
(1) prove its <strong>the</strong>re, and<br />
(2) actually begin to c<strong>on</strong>strain its n<strong>at</strong>ure<br />
Much work to be d<strong>on</strong>e :<br />
<br />
<br />
<br />
<br />
Modeling observ<strong>at</strong>i<strong>on</strong>s : covering factors, columns,<br />
velocity distributi<strong>on</strong>s, etc.<br />
Self-c<strong>on</strong>sistently model feedback gener<strong>at</strong>i<strong>on</strong><br />
Include radio and “quasar” mode feedback<br />
Incorpor<strong>at</strong>e into cosmological models<br />
But <strong>the</strong>re appears to be rapid progress!