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Lecture 5 - University of Waterloo

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Testing the No-Hair Theorem<br />

with Observations <strong>of</strong> Black Holes<br />

in the Electromagnetic Spectrum<br />

Tim Johannsen<br />

CITA National Fellow<br />

<strong>University</strong> <strong>of</strong> <strong>Waterloo</strong>/Perimeter Institute


Testing the No-Hair Theorem Observationally<br />

Kerr black hole?<br />

Something else?<br />

‣ Expand spacetime in multipole moments (mass M, spin a, …)<br />

‣ Parameterize quadrupole moment:<br />

‣ Use observations to measure (at least) 3 moments<br />

‣ Check whether:<br />

q ( a<br />

2 )<br />

i.e.: 0<br />

2<br />

q a<br />

Ryan 1995, 1997a,b<br />

Barack & Cutler 2004, 2007<br />

Collins & Hughes 2004<br />

Glampedakis & Babak 2006<br />

Brink 2008, 2009<br />

Gair et al. 2008<br />

Li & Lovelace 2008<br />

Will 2008<br />

Vigeland & Hughes 2010<br />

Johannsen & Psaltis 2010a, 2011b<br />

Vigeland et al. 2011


A New Metric for Rapidly Spinning Black Holes<br />

2 2Mr<br />

<br />

4aMr<br />

sin<br />

ds 1<br />

<br />

)<br />

<br />

<br />

<br />

<br />

a<br />

<br />

sin<br />

<br />

where<br />

2<br />

1<br />

h(<br />

r,<br />

)<br />

dt<br />

1<br />

h(<br />

r,<br />

dtd<br />

1<br />

h(<br />

r,<br />

)<br />

2 2<br />

2<br />

h(<br />

r,<br />

)sin<br />

<br />

<br />

r<br />

<br />

2<br />

dr<br />

<br />

d<br />

<br />

h(<br />

r,<br />

)<br />

<br />

2 2<br />

2<br />

4<br />

2 2 2 2a<br />

Mr sin a ( 2Mr)<br />

sin<br />

a<br />

<br />

<br />

<br />

<br />

2<br />

d<br />

<br />

<br />

<br />

r<br />

2<br />

2Mr<br />

a<br />

2<br />

r a<br />

2 2 cos<br />

2<br />

<br />

h(<br />

r,<br />

)<br />

<br />

3<br />

rM<br />

2<br />

<br />

3<br />

Johannsen & Psaltis 2011, PRD, 83, 124015


Quadrupole Effects:<br />

1. Location <strong>of</strong> the ISCO 2. Lightbending<br />

Johannsen & Psaltis 2011b, PRD, 83, 124015<br />

Johannsen 2012, Adv. Astron., 2012, 1


1. Imaging the Shadow <strong>of</strong> Sgr A*<br />

Inclination Angle: 68 o +5 o<br />

Spin: 0.0<br />

Spin Position Angle: -52 o<br />

-20 o<br />

+0.64<br />

+17 o<br />

-15 o<br />

Broderick, Fish, Doeleman, Loeb 2011, ApJ, 735, 110<br />

• Assume Kerr black hole in ADAF/RIAF model<br />

Broderick et al. 2009, ApJ, 697, 1164<br />

• Current VLBI data (JCMT – CARMA – SMT)<br />

Doeleman et al. 2008, Nature, 455, 78; Fish et al. 2011, ApJ, 727, 36


Broderick, Johannsen, Loeb, Psaltis 2012<br />

Testing the No-Hair Theorem with Sgr A*<br />

= 0.4 = -0.8<br />

Shape <strong>of</strong> shadow depends uniquely on mass, spin, disk inclination<br />

...as well as on quadrupole moment<br />

e.g., Falcke et al. 2000, ApJ, 528, L13<br />

Johannsen & Psaltis 2010b, ApJ, 718, 446


Bright Emission Ring!<br />

e.g., Beckwith & Done 2005, MNRAS, 359, 1217<br />

The Photon Ring<br />

clearly distinguishable<br />

independent <strong>of</strong><br />

flow properties<br />

‣ ideal for imaging!<br />

Johannsen & Psaltis 2010b, ApJ, 718, 446


Moscibrodzka et al. 2009,<br />

ApJ, 706, 497<br />

Shcherbakov & Penna 2011,<br />

ASP Conf. Ser., 439, 372<br />

Dexter et al. 2009, ApJ, 703, L142<br />

Photon Rings<br />

A ubiquitous signal,<br />

independent <strong>of</strong> the details<br />

<strong>of</strong> the accretion flow


Broderick, Johannsen, Loeb, Psaltis 2012<br />

Johannsen & Psaltis 2010a, ApJ, 716, 187


Broderick, Johannsen, Loeb, Psaltis 2012<br />

Johannsen & Psaltis 2010a, ApJ, 716, 187


Broderick, Johannsen, Loeb, Psaltis 2012<br />

Johannsen & Psaltis 2010a, ApJ, 716, 187


Independent Measurement: M, a, ε (mod i)<br />

Johannsen & Psaltis 2010b, ApJ, 716, 187<br />

Diameter:<br />

Displacement:<br />

Asymmetry:<br />

measures mass<br />

measures spin<br />

measures quadrupole moment


Combined Mass Measurement <strong>of</strong> Sgr A*<br />

Johannsen, Psaltis, Gillessen, Marrone, Ozel, Doeleman, & Fish 2012, ApJ, 758, 30<br />

Planned VLBI array: JCMT, CARMA, SMT, ALMA, SPT, SMA


Millimetron<br />

RadioAstron Newsletter Dec. 8, 2011<br />

VLBI from Space


Masses <strong>of</strong> other SMBHs with VLBI<br />

5-telescope<br />

array<br />

Millimetron<br />

mission<br />

Johannsen et al., ApJ, 758, 30


Galactic BHs and AGN<br />

from Gou et al. 2011, ApJ, 742, 85


Iron K- and L- Lines<br />

in 1H0707-495<br />

Fabian et al. 2009, Nature, 459, 540


2. Relativistically Broadened Iron Lines<br />

Johannsen & Psaltis, arXiv:1202.6069<br />

Psaltis & Johannsen, 2012, ApJ, 745, 1


Required Precision for Future Instruments<br />

Inclination 30 o<br />

Inclination 60 o<br />

Johannsen & Psaltis, arXiv:1202.6069


Observational Tests <strong>of</strong> the No-Hair Theorem<br />

1. VLBI-Imaging <strong>of</strong> Sgr A*<br />

Event Horizon Telescope<br />

2. Fluorescent Iron Lines<br />

e.g., ASTRO-H, ATHENA<br />

ASTRO-H<br />

3. Variability<br />

Need Timing Mission to detect higher<br />

order harmonics and resolve model<br />

degeneracies.<br />

e.g., LOFT

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