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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.

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