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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 37<br />

Figure 2.8 – Histograms <strong>of</strong> masses and ages for the sample <strong>of</strong> YSOs <strong>in</strong> Serpens, derived from the<br />

models <strong>of</strong> Baraffe et al. (1998) (top) and Siess et al. (2000) (bottom).<br />

from the stellar spectra (ages and masses) and their positi<strong>on</strong>s <strong>in</strong> the cloud were found.<br />

This analysis will be revisited <strong>on</strong>ce the entire sample <strong>of</strong> 150 YSOs will be available.<br />

Recent analysis suggests that the distance to Serpens may be as low as 193 ± 13<br />

pc (J. Knude, private communicati<strong>on</strong>), rather than the distance <strong>of</strong> 259 pc assumed<br />

here. <strong>The</strong> smaller distance would imply a notable <strong>in</strong>crease <strong>in</strong> <strong>in</strong>dividual ages due to<br />

the decrease <strong>in</strong> lum<strong>in</strong>osities, with median ages <strong>of</strong> 15.9 Myr and 10.1 Myr with the<br />

Baraffe et al. (1998) and Siess et al. (2000) tracks, respectively. Median masses are<br />

not so str<strong>on</strong>gly affected due to the mass tracks be<strong>in</strong>g almost vertical <strong>in</strong> the low-mass<br />

regime, yield<strong>in</strong>g median masses <strong>of</strong> 0.8 M ⊙ and 0.6 M ⊙ accord<strong>in</strong>g to the Baraffe et al.<br />

(1998) and Siess et al. (2000) tracks, respectively.<br />

2.7 Accreti<strong>on</strong> Based <strong>on</strong> Hα Emissi<strong>on</strong><br />

A relati<strong>on</strong> between the Hα l<strong>in</strong>e-to-c<strong>on</strong>t<strong>in</strong>uum ratio and evoluti<strong>on</strong> <strong>of</strong> its emitt<strong>in</strong>g source<br />

has been widely explored (Bertout 1989, Hartmann 1998, Muzerolle et al. 2003, White<br />

& Basri 2003, Stahler & Palla 2004, Natta et al. 2004). It is argued that the strength<br />

<strong>of</strong> the Hα l<strong>in</strong>e decreases with evoluti<strong>on</strong>ary stage. A similar decl<strong>in</strong>e is seen <strong>in</strong> the<br />

strength <strong>of</strong> the prom<strong>in</strong>ent Ca ii H and K l<strong>in</strong>es (3968 Å and 3934 Å, respectively)<br />

and <strong>in</strong> the surface rotati<strong>on</strong>al velocity, re<strong>in</strong>forc<strong>in</strong>g the motivati<strong>on</strong> for a chromospheric<br />

orig<strong>in</strong> for ma<strong>in</strong>-sequence Hα emissi<strong>on</strong>. However, active T Tauri stars have Hα fluxes<br />

much larger than those predicted by chromospheric models (Stahler & Palla 2004),<br />

mean<strong>in</strong>g that for these objects Hα is unlikely to orig<strong>in</strong>ate primarily <strong>in</strong> a chromosphere.<br />

Mass accreti<strong>on</strong> from a circumstellar disk is thought to be resp<strong>on</strong>sible for the excess

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