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Annual Report 2011 Max Planck Institute for Astronomy

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56 III. Selected Research Areas<br />

III.3 Dynamics of Galaxies: inferring their mass distribution and <strong>for</strong>mation history<br />

What is the distribution of luminous and dark matter<br />

in galaxies? How much of the <strong>for</strong>mation history of galaxies<br />

has been preserved in their internal dynamical<br />

structure? Is the mass of a central black hole correlated<br />

with the mass of the host galaxy? Is the concordance<br />

cosmological model in agreement with these findings<br />

on the scales of galaxies? These key questions regarding<br />

galaxy <strong>for</strong>mation in a cosmological context can be<br />

answered by studying the dynamics of galaxies. Here<br />

we present our research in this area.<br />

Kinematic tracers<br />

The motion or kinematics of astronomical objects is sensitive<br />

to the underlying gravitational potential, which<br />

is related, through Poisson’s equation, to the density<br />

of all matter, including any possible dark components.<br />

Consider, <strong>for</strong> example, gas moving in a circular orbit at<br />

radius R in the equatorial plane of a galaxy. The mass<br />

of the galaxy enclosed within this radius M ( R) determines<br />

the circular velocity V c (R) of the gas, because<br />

G M ( R)/R V c 2 , with G Newton’s constant of gravity.<br />

This means that if we can measure the gas velocity<br />

over a range of radii, we can infer the distribution of the<br />

galaxy’s total mass, i.e., including any possible contribution<br />

from unseen components.<br />

This is illustrated in Fig. III.3.1 <strong>for</strong> the elliptical galaxy<br />

NGC 2974. The top panel shows the projected stellar<br />

distribution, while the middle panel shows the velocity<br />

field of gas in the outer and inner parts. Red/blue<br />

indicates gas moving away/toward us along our lineof-sight,<br />

while green indicates gas that is moving in the<br />

plane of the sky. Taking out these projection effects, the<br />

red circles with error bars in the bottom panel show the<br />

Fig. III.3.1: Dark matter in the elliptical galaxy NGC 2974. Top:<br />

Digital Sky Survey optical image showing the projected stellar<br />

distribution. Middle: Gas velocity map of the outer parts<br />

via atomic hydrogen HI gas obtained with the VLA radiointerferometer,<br />

and of the inner parts via ionized [OIII] gas<br />

obtained with the sauroN integral-field spectrograph. Red/blue<br />

indicates gas moving away/toward along our line-of-sight,<br />

while green indicates gas that is moving in the plane of the sky.<br />

Bottom: The resulting circular velocity curve of red circles with<br />

error bars clearly shows that the gas and stars alone cannot explain<br />

the corresponding total mass distribution. Adding a dark<br />

matter halo which is consistent with cosmological simulations<br />

can explain the observations as indicated by the upper black<br />

solid line. (Extracted from Weijmans, Krajnović, van de Ven et<br />

al. 2008, MNRAS, 383, 1343).<br />

Declination (J2000)<br />

y<br />

V c [km/s]<br />

–340<br />

–42<br />

–44<br />

150<br />

100<br />

50<br />

0<br />

–50<br />

–100<br />

–150<br />

400<br />

300<br />

200<br />

100<br />

9h42m45s 40s 35s 30<br />

Right Ascension (J2000)<br />

s 25s 20s –100<br />

–50<br />

Sauron V [OIII]<br />

0<br />

0<br />

0 20 40 60<br />

radius<br />

x<br />

50<br />

n [km/s]<br />

300<br />

200<br />

100<br />

0<br />

–100<br />

–200<br />

–300<br />

100 150<br />

halo<br />

stars<br />

gas<br />

Credit: Weijmans, Krajnović, van de Ven<br />

80 100 120

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