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Extragalactic Astronomy and Cosmology: An Introduction

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9. The Universe at High Redshift<br />

400<br />

displayed, obtained from semi-analytic models. Massive<br />

halos which have formed early in cosmic history<br />

are currently found predominantly in the centers of very<br />

massive galaxy clusters. Assuming that the luminous<br />

QSOs at z ∼ 6 are harbored in the most massive halos<br />

of this epoch, we can deduce that these may today<br />

be identified as the central galaxies in clusters. This<br />

may provide an explanation as to why so many central,<br />

dominating cluster galaxies show AGN activity,<br />

though with a smaller luminosity due to small accretion<br />

rates.<br />

Abundance <strong>and</strong> Evolution of Supermassive Black<br />

Holes. Within the framework of these models, predictions<br />

are also made about the statistical evolution of<br />

SMBHs in the cores of galaxies. When two galaxies<br />

merge, their SMBHs will also coalesce after some time,<br />

where an accurate estimate for this time-scale is difficult<br />

to obtain. Owing to the high initial orbital angular<br />

momentum, the two SMBHs are, at the beginning of<br />

a merger, on an orbit with rather large mutual separation.<br />

By dynamical friction (see Sect. 6.2.6), caused by<br />

the matter distribution in the newly formed galaxy, the<br />

pair of SMBHs will lose orbital energy after the merger<br />

of the galaxies, <strong>and</strong> the two black holes will approach<br />

each other. Since this process takes a relatively long<br />

time, <strong>and</strong> since a massive galaxy will, besides a few<br />

major mergers, undergo numerous minor mergers, it is<br />

conceivable that many of the black holes that were originally<br />

the nuclei of low-mass satellite galaxies are today<br />

still on orbits at relatively large distances from the center<br />

of galaxies.<br />

In this model, phases in the evolution of galaxies exist<br />

in which two SMBHs are located close to the center.<br />

Indeed, there are a number of indications that such galaxies<br />

are actually observed. For instance, galaxies with<br />

two active nuclei have been found. Also a class of radio<br />

sources exists with an X-shaped morphology (instead<br />

of the usual bipolar radio structure), which can be interpreted<br />

as pairs of active SMBHs. Another signature<br />

of a binary system of SMBHs would be a periodicity<br />

in the emission, reflecting the orbital period. In some<br />

AGNs, periodic variations in the brightness have in fact<br />

been detected, the blazar OJ 287 being the best known<br />

example, with a period of 11.86 years.<br />

When two SMBHs merge, the initially wide orbit<br />

shrinks, in the final stages due to the emission of gravitational<br />

waves. This will cause the orbits to become<br />

more circular, as well as a decrease of the separation of<br />

the two black holes. According to the theory of black<br />

holes, there is a closest separation at which an orbit still<br />

is stable. Once the separation has shrunk to that size, the<br />

merging occurs, accompanied by a burst of gravitational<br />

wave emission. If the two SMBHs have the same mass,<br />

each of them will emit the same amount of gravitational<br />

wave energy, but in opposite directions, so that the net<br />

amount of momentum carried away by the gravitational<br />

waves is zero. However, if the masses are not equal, this<br />

cancellation no longer occurs, <strong>and</strong> the waves carry away<br />

a net linear momentum. According to momentum conservation,<br />

this will yield a recoil to the merged SMBH,<br />

<strong>and</strong> it will therefore move out of the galactic nucleus.<br />

Depending on the recoil velocity, it may return to the<br />

center in a few dynamical time-scales. However, if the<br />

recoil velocity is larger than the escape velocity from<br />

the galaxy, it may actually escape from the gravitational<br />

potential <strong>and</strong> become an intergalactic black hole. The<br />

importance of this effect is not quantitatively known,<br />

since the amplitude of the recoil velocity as determined<br />

from theoretical models is uncertain. It is zero for equal<br />

masses, <strong>and</strong> very small if one of the black hole masses<br />

is much smaller than the other. The recoil velocity attains<br />

a maximum value when the mass ratio of the two<br />

SMBHs is about 1/3.<br />

The mass increase of SMBHs in the course of cosmic<br />

history then has two different origins, first the merging<br />

with other low-mass SMBHs as a consequence of<br />

merger events, <strong>and</strong> second the accretion of gas that<br />

leads to the activity of SMBHs. Hierarchical models<br />

of galaxy evolution with central SMBHs are able to<br />

both reproduce, under certain assumptions, the correlation<br />

(see Sect. 3.5.3) between the SMBH mass <strong>and</strong><br />

the properties of the spheroidal stellar component, <strong>and</strong><br />

to successfully model the integrated AGN luminosity<br />

<strong>and</strong> the redshift-dependent luminosity function of<br />

AGNs.<br />

In the course of the merger of two SMBHs, an intense<br />

emission of gravitational waves will occur in the final<br />

phase. The space project LISA, which is planned to be<br />

launched sometime after 2013, is capable of observing<br />

the emission of gravitational waves from such merger<br />

processes, essentially throughout the visible Universe.<br />

Hence, it will become possible to directly trace the<br />

merger history of galaxies.

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