recoiling black holes in galactic centers michael boylan-kolchin, chung-pei ma, and eliot quataert...
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RECOILING BLACK HOLES IN GALACTIC CENTERS
Michael Boylan-Kolchin, Chung-Pei Ma, and Eliot Quataert (UC Berkeley)
astro-ph/0407488
Outline
• supermassive black hole binary formation and coalescence
• gravitational radiation recoil
• effects of recoil on stellar distributions
• comparison with early-type galaxies
Supermassive Black Holes and LCDM
• hierarchical cosmology + SMBH=black hole binaries
• tdf << tH only for major mergers
• BH coalescence rate determined by both cosmological and galactic physics: galaxy merger rate BH merger rate!
Why 1 parsec should matter to a cosmologist
if ab shrinks by a factor of ~150, gravitational wave emission causes rapid coalescence
)2010( MProblem: need mass of stars
…but loss cone only contains enough stars to reduce
ab by a factor of ~10 (i.e. M)
How? gravitational slingshot
Gravitational Radiation Recoil
• Anisotropic emission of gravitational waves gives a “kick” to the newly-formed BH
• Recoil velocity depends on BH mass ratio, BH spins, and spin alignment
• Recoil velocity can reach 100-500 km/s (Favata et al. 2004)
• Many consequences - Merritt et al.; Madau & Quataert; Haiman (all 2004)
Does radiation recoil have observable effects on elliptical galaxies?
• Plan: use purely gravity N-Body experiments (GADGET) to study the effects of gravitational radiation recoil
• simulate a kicked black hole, and follow the evolution of the stellar density and velocity profiles and trajectory of the black hole
E8
1)E(
E
02
2
2
d
d
df
r
GM
ar
GMr BH*)(
Initial ConditionsUse the equilibrium distribution function to set up the particles’ phase space coordinates:
33*
)/1(
1
2)(
arr
a
a
Mr
MBH=0
MBH=M*/300
Effects on the Stellar Density
M*=1010 Msun, a=1 kpc:
vesc=293 km/s=2.82 vcirc
tdyn=26 Myr
rh=0.089 a=89 pc
Additional Effects
• flattened density profile core in surface brightness profile
• small change of the inner velocity dispersion
• effects should be largest in galaxies with smallest vcirc(a)/vesc and for largest MBH/M
So why do “power-law” ellipticals (without central cores) exist?
• power-law galaxies are typically less massive than “core” ellipticals, so the effect of a kick should be more pronounced
• power-law galaxies seem to host central black holes
Does gas play a role?
• Faber et al. (1997): gas-rich mergers could lead to power-law galaxies
• problem: requires that starburst duration is long enough to counteract both binary coalescence effects and radiation recoil effects
• solution: can gas accelerate the coalescence process?
Conclusions
• supermassive BHs + hierarchical cosmology = binary black holes
• radiation recoil can lead to cores in stellar systems analogous to those seen in some early type galaxies
• gas may play an important role in enabling binary BHs to coalesce; in turn, this may help explain the existence of power-law early-type galaxies that form hierarchically