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174 Spectral Energy Distributi<strong>on</strong>s <strong>of</strong> the Young Stars with Disks <strong>in</strong> Serpens<br />

Figure 7.3 – Fracti<strong>on</strong>al disk lum<strong>in</strong>osity (L disk /L star) derived for the objects <strong>in</strong> Serpens (top left),<br />

compared to those <strong>in</strong> Taurus (bottom left), Upper Scorpius (top right) and η Chamaele<strong>on</strong>tis (bottom<br />

right). <strong>The</strong> dashed l<strong>in</strong>e <strong>in</strong> the Serpens distributi<strong>on</strong> accounts for completeness (see text for details).<br />

<strong>The</strong> boundary for accret<strong>in</strong>g vs. passive disks is put at L disk /L star ∼ 0.2. Thus “accret<strong>in</strong>g disks”<br />

does not refer to the <strong>in</strong>formati<strong>on</strong> <strong>on</strong> accreti<strong>on</strong> rates derived from Hα.<br />

Furthermore, Figure 7.3 shows the distributi<strong>on</strong> <strong>of</strong> L disk /L star <strong>in</strong> the Upper Scorpius<br />

and η Chamaele<strong>on</strong>tis clusters for the entire samples (c<strong>on</strong>sist<strong>in</strong>g <strong>of</strong> objects with<br />

IR-excess and those that have little or no excess, Maud et al. <strong>in</strong> prep). <strong>The</strong>se older<br />

regi<strong>on</strong>s are known to have lower disk fracti<strong>on</strong>s (Hernández et al. 2008), mean<strong>in</strong>g<br />

that most <strong>of</strong> the member stars have already fully dissipated their disks. Figure 7.3<br />

clearly shows this difference <strong>in</strong> relati<strong>on</strong> to the young Serpens and Taurus clouds, with<br />

distributi<strong>on</strong>s that peak (and spread) at c<strong>on</strong>siderably lower disk lum<strong>in</strong>osities. <strong>The</strong><br />

vertical dotted l<strong>in</strong>es roughly separate lum<strong>in</strong>osity ratios that can be expla<strong>in</strong>ed by different<br />

mechanisms: accreti<strong>on</strong> disks (L disk /L star > 0.2, Keny<strong>on</strong> & Hartmann 1987)<br />

and passive disks. “Debris”-like disks are c<strong>on</strong>siderably fa<strong>in</strong>ter (L disk /L star < 0.001).<br />

It is important to note that the L disk /L star distributi<strong>on</strong>s <strong>in</strong> Taurus, Upper Sco<br />

and η Cha are fairly complete. That is, for these well studied regi<strong>on</strong>s <strong>in</strong>formati<strong>on</strong> <strong>on</strong><br />

the entire young star populati<strong>on</strong> is available whether or not the source has IR excess<br />

(down to the brown dwarf limit, which ensures completeness for the results derived<br />

here for T Tauri stars). Taurus <strong>in</strong>deed has a brighter disk populati<strong>on</strong> than Upper Sco<br />

and η Cha. <strong>The</strong> Serpens sample presented here, <strong>on</strong> the other hand, is flux-limited<br />

and selected based <strong>on</strong> IR excess. That means that, by def<strong>in</strong>iti<strong>on</strong> <strong>of</strong> the selecti<strong>on</strong><br />

criteria, stars without disks and with disks fa<strong>in</strong>ter than 3 mJy at 8 µm are not part<br />

<strong>of</strong> the sample and therefore not shown <strong>in</strong> Figure 7.3. A c<strong>on</strong>servative calculati<strong>on</strong> <strong>of</strong><br />

the fracti<strong>on</strong>al disk lum<strong>in</strong>osity <strong>of</strong> the 88 missed sources (c<strong>on</strong>sider<strong>in</strong>g a flux lower than<br />

3 mJy at 8 µm) was performed and is shown <strong>on</strong> top <strong>of</strong> the distributi<strong>on</strong> <strong>of</strong> Serpens <strong>in</strong>

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