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Max Planck Institute for Astronomy - Annual Report 2007

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58 II. Highlights<br />

NGC5055 (M63) NGC628 (M74)<br />

NGC3031 (M81) NGC5194 (M51)<br />

Fig. II.8.2: Several examples of the galaxies observed within<br />

the tH i N g s project; left (this page): Spiral galaxies; right (Page<br />

59): Dwarf galaxies. The radio maps are coded in blue; with<br />

an overlay of infrared images (coded in yellow, they show the<br />

then approximate a constant value as the distance to the<br />

core region grows. The curves of faint galaxies slowly<br />

increase and do not reach a constant level within the<br />

HI area.<br />

Mass models of the galaxies, including dark matter,<br />

could be obtained from the measured rotation curves<br />

and these could be related to the baryonic masses derived<br />

from the sp i t z e r data. Here it became clear that in<br />

bright galaxies the influence of dark matter increases as<br />

the radius grows but that the ratio of dark to baryonic<br />

matter is never as large as in faint galaxies. Bright gal-<br />

distribution of the old stars) and a combination of infrared and<br />

ultraviolet (coded in violet, they show the distribution of the<br />

star <strong>for</strong>mation regions).<br />

axies are thus not so strongly dominated by dark matter<br />

as faint galaxies, and in particular dwarf galaxies. In the<br />

latter, the dark matter comprises over 90 percent of the<br />

total matter.<br />

With the existing data, the group then approached the<br />

question of the mass distribution of dark matter. Would<br />

it be possible to distinguish between the “cuspy core”<br />

model and the “soft core” model as was suggested by<br />

observations?<br />

Fig. II.8.5 shows all rotation curves (grey) as well<br />

as an averaged curve (black squares). Furthermore, the

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