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Observational Constraints on The Evolution of Dust in ...

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Evoluti<strong>on</strong> <strong>of</strong> <strong>Dust</strong> <strong>in</strong> Protoplanetary Disks 39<br />

Figure 2.9 – C<strong>on</strong>t<strong>in</strong>uum-subtracted pr<strong>of</strong>iles <strong>of</strong> Hα emissi<strong>on</strong> l<strong>in</strong>es. <strong>The</strong> solid gray l<strong>in</strong>es are the<br />

Gaussian fit to each pr<strong>of</strong>ile; dashed gray l<strong>in</strong>es mark the center <strong>of</strong> the Gaussian. (A color versi<strong>on</strong> <strong>of</strong><br />

this figure is available <strong>in</strong> the <strong>on</strong>l<strong>in</strong>e journal)<br />

2.7.2 Full Width <strong>of</strong> Hα at 10%<br />

Due to the uncerta<strong>in</strong>ties <strong>in</strong> the determ<strong>in</strong>ati<strong>on</strong> <strong>of</strong> EW[Hα] <strong>in</strong> low-resoluti<strong>on</strong> spectra,<br />

White & Basri (2003) proposed the full width <strong>of</strong> Hα at 10% <strong>of</strong> the peak <strong>in</strong>tensity<br />

(Hα[10%]) as an alternative to dist<strong>in</strong>guish CTTSs from WTTSs. <strong>The</strong>y found that<br />

stars with Hα[10%] greater than 270 km s −1 are CTTSs, <strong>in</strong>dependent <strong>of</strong> spectral<br />

types.<br />

We fitted Gaussian pr<strong>of</strong>iles to the Hα l<strong>in</strong>es (shown <strong>in</strong> Figure 2.9) <strong>in</strong> order to<br />

determ<strong>in</strong>e the Hα[10%]. <strong>The</strong> errors were calculated by propagat<strong>in</strong>g the error <strong>on</strong> the<br />

spectral resoluti<strong>on</strong> and the error <strong>of</strong> the Gaussian fit to the Hα l<strong>in</strong>e. <strong>The</strong> measured<br />

FWHM <strong>of</strong> each pr<strong>of</strong>ile was dec<strong>on</strong>volved assum<strong>in</strong>g a Gaussian <strong>in</strong>strumental pr<strong>of</strong>ile.<br />

Because <strong>of</strong> the low resoluti<strong>on</strong> <strong>of</strong> our spectra (183.6 km s −1 for WYFFOS, 126 km s −1<br />

for DOLORES, and 100 km s −1 for CAFOS), very narrow pr<strong>of</strong>iles (e.g., objects 106<br />

and 150) are unresolved.<br />

In spite <strong>of</strong> the low resoluti<strong>on</strong>, the Hα pr<strong>of</strong>iles found are broad enough <strong>in</strong> most<br />

cases to allow the extracti<strong>on</strong> <strong>of</strong> velocity <strong>in</strong>formati<strong>on</strong>, although with low accuracy.

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