Max Planck Institute for Astronomy - Annual Report 2007
Max Planck Institute for Astronomy - Annual Report 2007
Max Planck Institute for Astronomy - Annual Report 2007
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56 II. Highlights<br />
II.8 Unique Galay Portraits with Th i n g s<br />
Under MPIA’s leadership using the Very Large Array<br />
(VLA), an international team of astronomers studied a<br />
total of 34 nearby galaxies in the light of atomic hydrogen’s<br />
21 cm line. The VLA is a radio interferometer<br />
located near Socorro (New Mexico). The project was<br />
designated “The HI Nearby Galaxy Survey” (Th i n g s) and<br />
has been the largest program of this type at the VLA. It<br />
delivered data that are unique from many points of view<br />
and which will be the foundation <strong>for</strong> many systematic<br />
studies. In an initial series of publications, MPIA astronomers<br />
and colleagues from other institutions studied<br />
the rotation curves of spiral and dwarf galaxies in order<br />
to understand more about the puzzling dark matter halos.<br />
In a subsequent study, they researched the connection<br />
between the density of interstellar matter and star <strong>for</strong>mation.<br />
Observations of atomic hydrogen’s (HI) 21 cm line have<br />
been considered <strong>for</strong> decades to be one of the best methods<br />
to study the structure and kinematics of the interstellar<br />
medium – both in our Milky Way system as well as<br />
in other galaxies. Compared to other radiation, this has a<br />
series of advantages. HI emission experiences no extinction<br />
through interstellar dust and is in almost all cases<br />
optically thin, so that one can immediately derive the<br />
density of the hydrogen gas from the measured intensity.<br />
In addition, the kinematics of the hydrogen gas can be<br />
ascertained by looking at the Doppler effect.<br />
Selecting Galaxies <strong>for</strong> Th i n g s<br />
Because of the comparatively large wavelength, one<br />
needs large telescope apertures to obtain a sufficient spatial<br />
resolution. The VLA interferometer (Fig. II.8.1) offers<br />
unique possibilities in this regard. The VLA worked<br />
<strong>for</strong> tH i N g s in three different configurations with antenna<br />
separations of between 35 m and 11.4 km. A high spectral<br />
resolution between 1.3 and 5.2 km/s and a high spatial<br />
resolution of 6 arc seconds was decisive <strong>for</strong> the project.<br />
Thus, astronomers had to go to the technical limits of the<br />
instrument.<br />
The principal goal of tH i N g s is to study key characteristics<br />
of galaxies across the entire Hu b b l e sequence (with<br />
the exception of starburst galaxies). Galaxy morphology,<br />
star <strong>for</strong>mation and evolution, as well as mass distribution<br />
are the main areas of interest (compare 2005 <strong>Annual</strong><br />
<strong>Report</strong>, p. 82).<br />
The selection of galaxies followed several criteria.<br />
They cover a wide range in their star <strong>for</strong>mation rates,<br />
absolute luminosities, and metallicities. Almost all gal-<br />
axies are targets of the sp i t z e r Infrared Nearby Galaxies<br />
Survey (si N g s) project’s catalogue in which the MPIA is<br />
also participating. So far, the Na s a sp i t z e r space telescope<br />
is the most efficient infrared observatory. si N g s<br />
studies the near and middle infrared dust characteristics<br />
of galaxies. At the same time, <strong>for</strong> many of the tH i N g s<br />
galaxies, observations by the American ga l e x space telescope<br />
and CO observations from the ir a m telescope are<br />
available. Thus, star <strong>for</strong>mation rates can be ascertained<br />
and compared with the characteristics of neutral hydrogen<br />
(see below). Most of these observation data have<br />
about the same angular resolution of 6 arcseconds and<br />
can there<strong>for</strong>e easily be compared to each other.<br />
There were also other criteria in selecting the galaxies.<br />
For example, all of them are in a distance range of 6 to 50<br />
million light years, resulting in a spatial resolution of 300<br />
to 1600 light years – which is significantly better than<br />
earlier observations. Galaxies from the Local Group were<br />
not included because their angular size in the sky is too<br />
large. In the end, 34 galaxies were selected requiring 500<br />
hours observing time <strong>for</strong> the detailed study of their light<br />
on the 21cm line (Fig. II.8.2). On the following pages we<br />
present two already published results.<br />
Rotation Curves and Models <strong>for</strong> Dark Matter Halos<br />
Since the 1970s, there have been more and more indications<br />
that galaxies are embedded in extended clouds<br />
(halos) of dark matter. This was derived from the galaxies’<br />
rotation curves. If the galaxies consisted exclusively<br />
of visible matter, then the stars and gas clouds would<br />
orbit the center in Keplerian orbits on which the orbital<br />
velocity would decrease as the distance from the center<br />
grew. Yet, after a certain radius, one observes an almost<br />
constant velocity extending into the outskirts of the galaxies,<br />
our Milky Way also has such a rotation curve. This<br />
phenomenon is explained by the gravitational effect of<br />
the dark matter halo.<br />
This dark matter must have already played a decisive<br />
role in the <strong>for</strong>mation of galaxies. In the early universe<br />
it created potential troughs in which normal, baryonic<br />
material accumulated and further condensed into galaxies.<br />
Modern computer simulations take into account the<br />
gravitational effect of the dark matter, though its further<br />
physical characteristics are widely unknown. However,<br />
a problem has recently emerged in these cosmological<br />
calculations: The theory predicted that the density, and<br />
thus also the gravitational potential of dark matter halos,<br />
increases very steeply toward the center (with r –1 to<br />
r –1.5 ). This is known as the “cuspy core” model. Galaxy<br />
rotation curves however can best be explained with a