The discovery of dark objects with masses MBH
106 to 109.5
M
in galactic
nuclei is secure. But are they BHs? Proof requires
measurement of relativistic velocities near the Schwarzschild radius,
rs
2 MBH /
(108
M
) AU. Even for
M 31, rs ~ 8
x 10-7 arcsec. HST spectroscopic resolution is only 0".d1.
The conclusion that we are finding BHs is based on physical arguments that BH
alternatives fail to explain the masses and high densities of galactic nuclei.
The most plausible BH alternatives are clusters of dark objects produced
by ordinary stellar evolution. These come in two varieties, failed stars and
dead stars. Failed stars have masses m*
0.08
M
. They never
get hot enough for the fusion reactions that power stars, i.e., the
conversion of hydrogen to helium. They have a brief phase of modest brightness
while they live off of gravitational potential energy, but after this, they
could be used to make dark clusters. They are called brown dwarf stars, and
they include planetary mass objects. Alternatively, a dark cluster could be
made of stellar remnants - white dwarfs, which have typical masses of 0.6
M
; neutron
stars, which typically have masses of ~ 1.4
M
, and
black holes with masses of several
M
. Galactic
bulges are believed to form
in violent starbursts, so massive stars that turn quickly into dark remnants
would be no surprise. It is not clear how one could make dark clusters with the
required masses and sizes, especially not without polluting the remaining stars
with more metals than we see. But in the absence of direct proof that the dark
objects in galactic nuclei are BHs, it is important to examine alternatives.
However, dynamical measurements tell us more than the mass of a potential
BH. They also constrain the maximum radius inside which the dark stuff must
live. Its minimum density must therefore be high, and this rules out the above
BH alternatives in our Galaxy and in NGC 4258. High-mass remnants such as white
dwarfs, neutron stars, and stellar BHs would be relatively few in number. The
dynamical evolution of star clusters is relatively well understood; in
the above
galaxies, a sparse cluster of stellar remnants would evaporate completely in
108
yr. Low-mass objects such as brown dwarfs would be so numerous
that collision times would be short. Stars generally merge when they collide.
A dark cluster of low-mass objects would become luminous because brown dwarfs
would turn into stars.
More exotic BH alternatives are not ruled out by such arguments. For example, the dark matter that makes up galactic halos and that accounts for most of the mass of the Universe may in part be elementary particles that are cold enough to cluster easily. It is not out of the question that a cluster of these could explain the dark objects in galaxy centers without getting into trouble with any astrophysical constraints. So the BH case is not rigorously proved. What makes it compelling is the combination of dynamical evidence and the evidence from AGN observations. This is discussed in the previous article.
For many years, AGN observations were decoupled from the dynamical evidence for BHs. This is no longer the case. Dynamical BH detections are routine. The search itself is no longer the main preoccupation; we can concentrate on physical questions. New technical developments such as better X-ray satellites ensure that progress on BH astrophysics will continue to accelerate.