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Max Planck Institute for Astronomy - Annual Report 2007

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60 II. Highlights<br />

V [km s –1 ] V c [km s –1 ]<br />

V [km s –1 ] V c [km s –1 ]<br />

150<br />

100<br />

50<br />

0<br />

–50<br />

100<br />

50<br />

0<br />

–50<br />

NGC2403<br />

0<br />

0<br />

V5<br />

IC2574<br />

V5<br />

200 400 600<br />

r<br />

200<br />

800 1000 1200<br />

It is still unclear today whether all galaxies or at least<br />

each galaxy type follows a universal “Schmidt Law” or<br />

whether varying external conditions significantly influence<br />

the relationship between star <strong>for</strong>mation rate and gas<br />

density. This question is of great significance <strong>for</strong> theories<br />

and models of galaxy evolution.<br />

If one experimentally pursues the question, then it<br />

turns out to be useful to distinguish between the density<br />

of atomic (HI) and molecular gas (H 2 ). tH i N g s is<br />

especially suitable because of the high spatial resolution<br />

that it can achieve and its homogenous sensitivity. An<br />

astronomer team with Frank Bigiel, Adam Leroy, and<br />

Fabian Walter discussed this question by using data from<br />

the ga l e x Nearby Galaxy Survey and si N g s. From these<br />

the star <strong>for</strong>mation rate could be derived. In addition, CO<br />

observations with the 30 m ir a m telescope were available<br />

r<br />

400 600<br />

Fig. II.8.3: These rotation curves (blue) demonstrate how strongly<br />

the derived radial velocities vary depending on the method<br />

applied; above: the rotation-dominated galaxy, NGC 2403;<br />

below: IC 2574, in which strongly asymmetrical line profiles<br />

appear.<br />

log(V halo / km s –1 )<br />

2.5<br />

2<br />

1.5<br />

1<br />

0<br />

0.5<br />

log (V/km s –1 )<br />

3<br />

2<br />

1<br />

0<br />

–22<br />

–20 –18<br />

M B [mag]<br />

log(r) = 1<br />

–16 –14<br />

Fig. II.8.4: The rotation curves of all galaxies, sorted by absolute<br />

luminosities of the galaxies with a logarithmic representation<br />

of the rotation velocity.<br />

which permitted the derivation of the molecular hydrogen’s<br />

(H 2 ) density.<br />

Fig. II.8.6 shows the results (above) <strong>for</strong> spiral galaxies<br />

with H 2 -dominated central areas as well as (below) <strong>for</strong><br />

late spiral and dwarf galaxies. The values are listed in relation<br />

to averaged radius and azimuth. One sees how star<br />

<strong>for</strong>mation rates and H 2 -density decrease in spiral galaxies<br />

with growing distance, while the HI density does not follow<br />

this trend. In Fig. II.8.7, these measurements <strong>for</strong> the<br />

spiral galaxies were then plotted such that the SFR can<br />

Fig. II.8.5: The studied galaxies’ rotation curves. tH i N g s measurements<br />

(red), their averages (blue squares), cosmological<br />

models (dotted curves), as well as a theoretical result by S. S.<br />

McGaugh et al. from <strong>2007</strong> (upper dotted curve).<br />

1<br />

log(R/kpc)<br />

1.5 2

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