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Annual Report 2011 Max Planck Institute for Astronomy

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dM (A v )<br />

1<br />

0.1<br />

0.01<br />

p (ln (A v / mag)) (normalized)<br />

1<br />

0.1<br />

0.01<br />

0.001<br />

0.0001<br />

2<br />

Cali<strong>for</strong>nia<br />

exp (–0.49 A v )<br />

A B C D F G H I J<br />

exp (–0.12 Av )<br />

10<br />

A B C D F G H I J<br />

filamentary IRDC called “The Snake”. The shadowing<br />

is caused by dust particles in the cloud that absorb the<br />

background radiation. From the amount of this absorption<br />

it is possible to estimate the mass of intervening<br />

dust, and hence, the mass distribution of the cloud.<br />

Kainulainen & Tan (submitted) presented a scheme<br />

<strong>for</strong> combining these two types of data, Nir extinction<br />

mapping with background stars and Mir extinction mapping<br />

with surface brightness data, into mass distribution<br />

data with unprecedented high sensitivity and spatial<br />

Av [mag]<br />

10 100<br />

2.5<br />

Orion B<br />

exp (–0.22 A v )<br />

Orion A<br />

exp (–0.18 A v )<br />

15<br />

Av [mag]<br />

20 25<br />

3 3.5<br />

ln (A v / mag)<br />

III.2 Formation of star-<strong>for</strong>ming structures in the interstellar medium 53<br />

4 4.5 5<br />

Fig. III.2.5.: Top: Column density PDFs of ten IRDCs (colored<br />

lines) and the nearby Ophiuchus star-<strong>for</strong>ming cloud (black<br />

dashed line). The shapes of the PDFs of the IRDCs are, on<br />

average, compatible with a log-normal function (shown with<br />

a dotted black line). Left: The cumulative <strong>for</strong>ms of the PDFs<br />

<strong>for</strong> the IRDCs (colored lines) and <strong>for</strong> three nearby molecular<br />

clouds (black dotted lines). The IRDCs contain somewhat<br />

more high-column density material than nearby clouds, which<br />

might reflect their location at smaller Galacto-centric radii, and<br />

hence, higher pressures.<br />

resolution. The bottom panels of Figure III.2.4 show as<br />

an example the mass distribution map derived <strong>for</strong> “The<br />

Snake”. The data reaches the resolution of 2, which<br />

at the distance of “The Snake” corresponds to about<br />

0.04 Pc.<br />

The high-dynamic-range data resulting from the new<br />

technique makes it possible not only to examine the<br />

column density PDFs in potential high-mass star-<strong>for</strong>ming<br />

sites, but also to examine the PDFs of molecular<br />

clouds over a greatly wider dynamic range than the data<br />

discussed in the context of low-mass clouds (see Fig.<br />

II.2.2). Figure III.2.5 shows the column density PDFs<br />

of 10 IRDCs and that of Ophiuchus, which is a typical<br />

nearby star-<strong>for</strong>ming cloud. The PDFs of IRDCs are<br />

quite similar to that of Ophiuchus (they extend to higher<br />

column densities because the dynamic range of their data<br />

is wider). This, first of all, suggests that star-<strong>for</strong>mation<br />

may have already started in the IRDCs. Indeed, some<br />

of the IRDCs included in Fig. III.2.5 show some typical<br />

star-<strong>for</strong>ming signs in the near-and mid-infrared, such<br />

as bubbles and reflection nebulae. However, finding out<br />

exactly how many young stars are currently <strong>for</strong>ming in<br />

Credit: J. Kainulainen

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