and Cosmology
Extragalactic Astronomy and Cosmology: An Introduction
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.