and Cosmology
Extragalactic Astronomy and Cosmology: An Introduction
Extragalactic Astronomy and Cosmology: An Introduction
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2. The Milky Way as a Galaxy<br />
74<br />
produce such a large number of white dwarfs as a final<br />
stage of stellar evolution, the total star formation<br />
in our Milky Way, integrated over its lifetime, needs<br />
to be significantly larger than normally assumed. In<br />
this case, many more massive stars would also have<br />
formed, which would then have released the metals they<br />
produced into the ISM, both by stellar winds <strong>and</strong> in supernova<br />
explosions. In such a scenario, the metal content<br />
of the ISM would therefore be distinctly higher than is<br />
actually observed. The only possibility of escaping this<br />
argument is with the hypothesis that the mass function<br />
of newly formed stars (the initial mass function, IMF)<br />
was different in the early phase of the Milky Way compared<br />
to that observed today. The IMF that needs to be<br />
assumed in this case is such that for each star of intermediate<br />
mass which evolves into a white dwarf, far fewer<br />
high-mass stars, responsible for the metal enrichment<br />
of the ISM, must have formed in the past compared<br />
to today. However, we lack a plausible physical model<br />
for such a scenario, <strong>and</strong> it is in conflict with the starformation<br />
history that we observe in the high-redshift<br />
Universe (see Chap. 9).<br />
Neutron stars can be excluded as well, because<br />
they are too massive (typically > 1M ⊙ ); in addition,<br />
they are formed in supernova explosions, implying that<br />
the aforementioned metallicity problem would be even<br />
greater for neutron stars. Would stellar-mass black holes<br />
be an alternative? The answer to this question depends<br />
on how they are formed. They could not originate in SN<br />
explosions, again because of the metallicity problem.<br />
If they had formed in a very early phase of the Universe<br />
(they are then called primordial black holes), this<br />
would be an imaginable, though perhaps quite exotic,<br />
alternative.<br />
However, we have strong indications that the<br />
interpretation of the MACHO results is not as straightforward<br />
as described above. Some doubts have been<br />
raised as to whether all events reported as being due to<br />
microlensing are in fact caused by this effect. In fact,<br />
one of the microlensing source stars identified by the<br />
MACHO group showed another bump seven years after<br />
the first event. Given the extremely small likelihood of<br />
two microlensing events happening to a single source<br />
this is almost certainly a star with unusual variability.<br />
As argued previously, by means of t E we only measure<br />
a combination of lens mass, transverse velocity,<br />
<strong>and</strong> distance. The result given in Fig. 2.29 is therefore<br />
based on the statistical analysis of the lensing events<br />
in the framework of a halo model that describes the<br />
shape <strong>and</strong> the radial density profile of the halo. However,<br />
microlensing events have been observed for which<br />
more than just t E can be determined – e.g., events in<br />
which the lens is a binary star, or those for which t E<br />
is larger than a few months. In this case, the orbit of<br />
the Earth around the Sun, which is not a linear motion,<br />
has a noticeable effect, causing deviations from the<br />
st<strong>and</strong>ard curve. Such parallax events have indeed been<br />
observed. 13 Three events are known in the direction of<br />
the Magellanic Clouds in which more than just t E could<br />
be measured. In all three cases the lenses are most likely<br />
located in the Magellanic Clouds themselves (an effect<br />
called self-lensing) <strong>and</strong> not in the halo of the Milky<br />
Way. If for those three cases, where the degeneracy between<br />
lens mass, distance, <strong>and</strong> transverse velocity can<br />
be broken, the respective lenses are not MACHOs in the<br />
Galactic halo, we might then suspect that in most of the<br />
other microlensing events the lens is not a MACHO either.<br />
Therefore, it is currently unclear how to interpret<br />
the results of the microlensing surveys. In particular, it<br />
is unclear to what extent self-lensing contributes to the<br />
results. Furthermore, the quantitative results depend on<br />
the halo model.<br />
The EROS collaboration used an observation strategy<br />
which was sightly different from that of the MACHO<br />
group, by observing a number of fields in very short time<br />
intervals. Since the duration of a lensing event depends<br />
on the mass of the lens as Δt ∝ M 1/2 – see (2.88) – they<br />
were also able to probe very small MACHO masses.<br />
The absence of lensing events of very short duration<br />
then allowed them to derive limits for the mass fraction<br />
of such low-mass MACHOs, as is shown in Fig. 2.30.<br />
Despite this unsettled situation concerning the interpretation<br />
of the MACHO results, we have to emphasize<br />
that the microlensing surveys have been enormously<br />
successful experiments because they accomplished<br />
exactly what was expected at the beginning of the observations.<br />
They measured the lensing probability in<br />
the direction of the Magellanic Clouds <strong>and</strong> the Galactic<br />
bulge. The fact that the distribution of the lenses differs<br />
from that expected by no means diminishes the success<br />
of these surveys.<br />
13 These parallax events in addition prove that the Earth is in fact<br />
orbiting around the Sun – even though this is not really a new insight.