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Untitled - Laboratoire d'Astrophysique de l'Observatoire de Grenoble

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2.2 µ m<br />

0.5"<br />

11.7 µ m<br />

Figure 6.1: Left Panel: K-band image of the edge-on disk HK Tauri B ontained with NACO/VLT. (image<br />

from Ménard et al. (2005), in prep.). Right panel: 12µm scattered light image of HK Tau B obtained with<br />

KECK/LWS. Image from McCabe et al. (2003)<br />

light at 4µm comes from a layer located twice as close to the ring midplane than the visible scattered light<br />

(see Figure 6.2). Combined with the need for larger grains to account for the scattering phase function in the<br />

thermal infrared, and the need for very small grains at the disk surface to account for the large polarisation<br />

observed (Silber et al. 2000, ApJ, 536, L89), this is the first direct evi<strong>de</strong>nce for the stratification of dust grains,<br />

possibly as a result of vertical settling. This settling is a necessary step for dust to accumulate in the disk<br />

midplane and to grow into planetesimals, i.e., to start forming larger bodies, eventually rocky cores of planets,<br />

in the disks.<br />

0.8 µ m 3.8 µ m<br />

1"<br />

Figure 6.2: Left Panel: HST/ACS F814W image of the circumbinary ring of GG Tau (image from Krist et al.<br />

2005, ApJ, in press). Right panel: 3.8uµm scattered light image obtained with KECK. Image from Duchêne<br />

et al. (2004)<br />

To further probe small grains, and whenever possible, polarimetric mapping is also obtained. However, due<br />

to the paucity of polarimetric data, studies have been completed only for a few sources so far. Silber et al.<br />

(2000, ApJ, 536, L89) presented to first polarisation of a disk (GG Tau). Glauser et al. (2005) in prep. are<br />

finalising the analysis for IRAS 04158+2805. Our group is one of the very few using that powerful property of<br />

light for disk studies.<br />

In a parallel approach to scattered light images, we pursue millimeter interferometric images of T Tauri<br />

82<br />

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