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Extragalactic Astronomy and Cosmology: An Introduction

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7. <strong>Cosmology</strong> II: Inhomogeneities in the Universe<br />

(<strong>and</strong> clusters), thus contributing to the density, but also<br />

these baryons have modified the density profile of dark<br />

matter halos in the course of cosmic evolution. Baryons<br />

are dissipative, they can cool, form a disk, <strong>and</strong> accrete<br />

inwards. The change in the resulting density distribution<br />

of baryons by dissipative processes cause a change of the<br />

gravitational potential over time, to which dark matter<br />

also reacts. The dark matter profile in real galaxies is<br />

thus modified compared to pure dark matter simulations.<br />

Despite these difficulties, it has been found that the<br />

X-ray data of many clusters are compatible with an<br />

NFW profile. Analyses based on the weak lensing effect<br />

also show that an NFW mass profile provides a very<br />

good description for shear data. In Fig. 7.16 it is shown<br />

that the radial profile of the galaxy density in clusters<br />

on average follows an NFW profile, where the mean<br />

concentration index is c ≈ 3, i.e., smaller than expected<br />

for the mass profile of clusters. One interpretation of this<br />

result is that the galaxy distribution in clusters is less<br />

strongly concentrated than the density of dark matter.<br />

7.5.5 The Substructure Problem<br />

As we will discuss in detail in the next chapter, the<br />

CDM model of cosmology has proven to be enormously<br />

successful in describing <strong>and</strong> predicting cosmological<br />

observations. Because this model has achieved this success<br />

<strong>and</strong> is therefore considered the st<strong>and</strong>ard model,<br />

results that apparently do not fit into the st<strong>and</strong>ard model<br />

are of particular interest. The rotation curves of LSB<br />

galaxies mentioned above are one such result. Either<br />

one finds a good reason for this apparent discrepancy<br />

between observation <strong>and</strong> the predictions of the<br />

CDM model or, otherwise, results of this kind indicate<br />

the necessity to introduce extensions to the CDM<br />

model. In the former case, the model would have overcome<br />

another hurdle in demonstrating its validity <strong>and</strong><br />

would be confirmed even further, whereas in the latter<br />

case, new insights would be gained into the physics of<br />

cosmology.<br />

Sub-Halos of Galaxies <strong>and</strong> Clusters of Galaxies.<br />

Besides the rotation curves of LSB galaxies, there is<br />

another observation that does not seem to fit into the<br />

picture of the CDM model at first sight. Numerical<br />

simulations of structure formation show that a halo of<br />

mass M contains numerous halos of much lower mass,<br />

Fig. 7.16. The galaxy distribution averaged over 93 nearby<br />

clusters of galaxies, as a function of the projected distance<br />

to the cluster center. Galaxies have been selected in the NIR,<br />

<strong>and</strong> cluster masses, <strong>and</strong> thus r 200 , have been determined from<br />

X-ray data. Plotted is the projected number density of cluster<br />

galaxies, averaged over the various clusters, versus the scaled<br />

radius r/r 200 . In the top panel the galaxy sample is split into<br />

luminous <strong>and</strong> less luminous galaxies, while in the bottom<br />

panel the cluster sample is split according to the cluster mass.<br />

The solid curves show a fit of the projected NFW profile,<br />

which turns out to be an excellent description in all cases. The<br />

concentration index is, with c ≈ 3, roughly the same in all<br />

cases, <strong>and</strong> smaller than expected for the mass profile of clusters<br />

so-called sub-halos. For instance, a halo with the mass<br />

of a galaxy cluster contains hundreds or even thous<strong>and</strong>s<br />

of halos with masses that are orders of magnitude lower.

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