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Observational Constraints on The Evolution of Dust in ...

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130 From Protoplanetary Disks to Planetary Systems<br />

protoplanetary disks are optically thick at optical and IR wavelengths, the silicate<br />

features observed <strong>in</strong> the mid-IR are generally emitted by dust <strong>in</strong> the optically th<strong>in</strong><br />

disk surface <strong>on</strong>ly. To probe the disk midplane, observati<strong>on</strong>s at l<strong>on</strong>ger wavelengths<br />

are necessary. Additi<strong>on</strong>ally, the emissi<strong>on</strong> at 10 and 20 µm has been shown to arise<br />

from different gra<strong>in</strong> populati<strong>on</strong>s, prob<strong>in</strong>g different radii (Kessler-Silacci et al. 2006;<br />

Ol<strong>of</strong>ss<strong>on</strong> et al. 2009, 2010). While the 10 µm feature probes a warmer dust populati<strong>on</strong>,<br />

at ≤ 1 AU for T Tauri stars, the dust emitt<strong>in</strong>g at 20 µm is colder, further out and<br />

deeper <strong>in</strong>to the disk (Kessler-Silacci et al. 2007).<br />

Two methods have been proposed to expla<strong>in</strong> the formati<strong>on</strong> <strong>of</strong> crystal gra<strong>in</strong>s: thermal<br />

anneal<strong>in</strong>g <strong>of</strong> amorphous gra<strong>in</strong>s or vaporizati<strong>on</strong> followed by gas-phase c<strong>on</strong>densati<strong>on</strong>.<br />

Both methods require high temperatures (above ∼1000 K, Fabian et al. 2000;<br />

Gail 2004) which is <strong>in</strong>c<strong>on</strong>sistent with outer disk temperatures. However, crystall<strong>in</strong>e<br />

gra<strong>in</strong>s have been observed <strong>in</strong> outer, as well as <strong>in</strong> <strong>in</strong>ner disks (van Boekel et al. 2004).<br />

Large-scale radial mix<strong>in</strong>g has been <strong>in</strong>voked to expla<strong>in</strong> the presence <strong>of</strong> crystals at low<br />

temperatures <strong>in</strong> the outer disk (Bockelée-Morvan et al. 2000; Gail 2004; Ciesla 2009).<br />

A third proposed formati<strong>on</strong> mechanism for crystal formati<strong>on</strong> is that shock waves could<br />

locally heat amorphous silicates and crystallize them (Desch & C<strong>on</strong>nolly 2002; Harker<br />

& Desch 2002).<br />

From protoplanetary disks to comets, several authors have attempted to <strong>in</strong>fer the<br />

dust compositi<strong>on</strong> from IRS spectra and laboratory data <strong>on</strong> amorphous and crystall<strong>in</strong>e<br />

silicate dust, us<strong>in</strong>g a variety <strong>of</strong> analysis techniques. Whether for <strong>in</strong>dividual objects<br />

(Forrest et al. 2004; Merín et al. 2007; P<strong>in</strong>te et al. 2008; Bouy et al. 2008), for mixed<br />

disk samples (Bouwman et al. 2001; Apai et al. 2005; van Boekel et al. 2005; Bouwman<br />

et al. 2008; Ol<strong>of</strong>ss<strong>on</strong> et al. 2009, 2010; Juhász et al. 2010), or systematic studies <strong>of</strong> the<br />

disk populati<strong>on</strong> <strong>of</strong> a given star-form<strong>in</strong>g regi<strong>on</strong> (Sicilia-Aguilar et al. 2009; Wats<strong>on</strong> et<br />

al. 2009; Sargent et al. 2009), it has been shown that a significant mass fracti<strong>on</strong> <strong>of</strong> the<br />

dust <strong>in</strong> those disks must be <strong>in</strong> crystall<strong>in</strong>e form. However, the many studies deal<strong>in</strong>g<br />

with the m<strong>in</strong>eralogical compositi<strong>on</strong> <strong>of</strong> dust to date focus <strong>on</strong> a specific regi<strong>on</strong> or object,<br />

fail<strong>in</strong>g to <strong>in</strong>vestigate the hypothesis that the crystall<strong>in</strong>ity fracti<strong>on</strong> is a measure <strong>of</strong> the<br />

evoluti<strong>on</strong>ary stage <strong>of</strong> a regi<strong>on</strong>. That is, no study <strong>in</strong> the literature has yet <strong>in</strong>vestigated<br />

an <strong>in</strong>crease <strong>of</strong> crystall<strong>in</strong>ity fracti<strong>on</strong> with cluster age.<br />

M<strong>in</strong>eralogical studies <strong>of</strong> Solar System bodies show a range <strong>of</strong> crystall<strong>in</strong>ity fracti<strong>on</strong>s.<br />

Evidence from primitive ch<strong>on</strong>drites shows that the abundance <strong>of</strong> crystall<strong>in</strong>e silicate<br />

material varies from nearly noth<strong>in</strong>g up to 20 – 30 % (e.g. Acfer 094 and ALH77307,<br />

P<strong>on</strong>toppidan & Brearley 2010 and references there<strong>in</strong>). Oort cloud comets, with l<strong>on</strong>g<br />

periods and large distances from the Sun, have <strong>in</strong>ferred crystall<strong>in</strong>ity fracti<strong>on</strong>s up to<br />

60 – 80 % (e.g. Hale-Bopp, Wooden et al. 1999, 2007). Jupiter-family, or short<br />

period comets, have lower fracti<strong>on</strong>s, up to ∼35 % (e.g. 9P/Tempel 1, Harvey et al.<br />

2007b; 81P/Wild 2, Zolensky et al. 2006). This discrepancy <strong>in</strong> fracti<strong>on</strong>s po<strong>in</strong>ts to the<br />

existence <strong>of</strong> a radial dependence <strong>in</strong> crystall<strong>in</strong>ity fracti<strong>on</strong> <strong>in</strong> the protoplanetary disk<br />

around the young Sun (Harker et al. 2005). It is important to note that those values<br />

are model dependent, and the use <strong>of</strong> large amorphous gra<strong>in</strong>s (10 – 100 µm) can lead<br />

to systematically lower crystall<strong>in</strong>e fracti<strong>on</strong>s (Harker et al. 2002). This is evident for

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