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Annual Report 2011 Max Planck Institute for Astronomy

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48 III. Selected Research Areas<br />

III.2 Formation of star-<strong>for</strong>ming structures in the interstellar medium<br />

New stars are born in the cold and dense molecular<br />

clouds that are present “everywhere” in the Universe.<br />

How these molecular clouds are <strong>for</strong>med and how they<br />

evolve are key questions in the current ef<strong>for</strong>ts to establish<br />

global laws that regulate the star <strong>for</strong>mation process.<br />

The fundamental physical processes that are responsible<br />

<strong>for</strong> the evolution of molecular clouds can be studied<br />

through accurate measurements of how the material in<br />

them is distributed. Here we review our research on<br />

this topic.<br />

Molecular clouds of the interstellar medium (ISM) provide<br />

the environments where new stars in the Universe<br />

can be born. There is an intricate, two-way connection<br />

between the physical structure of molecular clouds and<br />

star <strong>for</strong>mation inside them. On the one hand, star <strong>for</strong>mation<br />

is very concretely driven by the molecular cloud<br />

structure: how much and how rapidly a cloud can <strong>for</strong>m<br />

stars depends crucially on how exactly the material in it<br />

Fig. III.2.1: Dust extinction map of the Ophiuchus star-<strong>for</strong>ming<br />

region. The dust extinction can be used as a tracer of the gas<br />

column density in molecular clouds, and hence, as a tracer of<br />

their mass distributions. In Kainulainen et al. (2009, A&A,<br />

508, L35) and Kainulainen et al. (<strong>2011</strong>, A&A, 530, A64), we<br />

derived extinction maps <strong>for</strong> 23 nearby molecular clouds and<br />

studied with the maps the probability distributions of column<br />

densities in them. Based on our findings in these works, we<br />

proposed a new evolutionary scheme <strong>for</strong> molecular clouds<br />

in which the pressure from the diffuse medium surrounding<br />

denser clumps in the clouds plays a significant role in the cloud<br />

evolution.<br />

Galactic latitude<br />

20<br />

16<br />

12<br />

10<br />

5 0<br />

Galactic longitude<br />

is organized. However on the other hand, the star-<strong>for</strong>mation<br />

process itself is a great sculptor of molecular clouds.<br />

Once started in the cloud, active star <strong>for</strong>mation will efficiently<br />

restructure the cloud material with jets and<br />

outflows from young stars, radiation pressure from massive<br />

stars, and powerful shock waves from dying stars.<br />

These processes rapidly erase the structural characteristics<br />

of the clouds that were prevalent be<strong>for</strong>e the star <strong>for</strong>mation<br />

started in them.<br />

How exactly the molecular clouds in the ISM come to<br />

be and what are the physics driving their <strong>for</strong>mation and<br />

evolution are fundamental open questions in the field<br />

of ISM- and star <strong>for</strong>mation-research today. One way to<br />

study these processes is borne out by the fact that different<br />

physical mechanisms cause the material in the clouds<br />

to be organized in different ways. There<strong>for</strong>e, accurate<br />

measurements of the clouds mass distribution lead to in<strong>for</strong>mation<br />

on what mechanisms are responsible <strong>for</strong> shaping<br />

the clouds.<br />

What regulates the structure-and star <strong>for</strong>mation in molecular<br />

clouds?<br />

We know today that the molecular clouds are <strong>for</strong>med and<br />

shaped primarily by the interplay of three <strong>for</strong>ces: the turbulent<br />

energy in the ISM, gravitational <strong>for</strong>ces, and the<br />

support of magnetic fields within them. Schematically,<br />

the pathway of gas in galaxies towards star <strong>for</strong>mation<br />

begins from large-scale instabilities, e.g. from atomic<br />

gas flows colliding at supersonic velocities, resulting<br />

in shocks, and further, to strong density fluctuations in<br />

7 deg = 15 pc<br />

355 350<br />

Credit: J. Kainulainen

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