Table C.1
Correlations between surviving disk and stellar properties at different ages of disk evolution considering the IMF.
| x | y | Time (Myr) | r | α | β |
|---|---|---|---|---|---|
| log10 R12CO,90% (AU) | log10 Mgas (M⊙) | 1 | ![]() |
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| 3 | ![]() |
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||
| 5 | ![]() |
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| 10 | ![]() |
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||
| log10 M⋆ (M⊙) | log10 Mgas (M⊙) | 1 | ![]() |
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| 3 | ![]() |
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||
| 5 | ![]() |
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||
| 10 | ![]() |
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||
| log10 M⋆ (M⊙) | log10 ϵ (= Mgas/M⋆) | 1 | ![]() |
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| 3 | ![]() |
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||
| 5 | ![]() |
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||
| 10 | ![]() |
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||
| log10 FUV (G0) | log10 Mgas (M⊙) | 1 | ![]() |
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| 3 | ![]() |
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||
| 5 | ![]() |
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||
| 10 | ![]() |
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||
| log10 M⋆ (M⊙) | log10 R12CO,90% (AU) | 1 | ![]() |
![]() |
![]() |
| 3 | ![]() |
![]() |
![]() |
||
| 5 | ![]() |
![]() |
![]() |
||
| 10 | ![]() |
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||
| log10 FUV (G0) | log10 R12CO,90% (AU) | 1 | ![]() |
![]() |
![]() |
| 3 | ![]() |
![]() |
![]() |
||
| 5 | ![]() |
![]() |
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||
| 10 | ![]() |
![]() |
![]() |
||
| log10 M⋆ (M⊙) | log10 FUV (G0) | 1 | ![]() |
![]() |
![]() |
| 3 | ![]() |
![]() |
![]() |
||
| 5 | ![]() |
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||
| 10 | ![]() |
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||
| log10 M⋆ (M⊙) | log10 Rc (AU) | 1 | ![]() |
![]() |
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| 3 | ![]() |
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||
| 5 | ![]() |
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||
| 10 | ![]() |
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||
| log10 M⋆ (M⊙) | log10 α | 1 | ![]() |
![]() |
![]() |
| 3 | ![]() |
![]() |
![]() |
||
| 5 | ![]() |
![]() |
![]() |
||
| 10 | ![]() |
![]() |
![]() |
||
Notes. Summary of the correlations and fits among different disk and stellar properties at 1, 3, 5 and 10 Myr using linmix (Kelly 2007). The fitting function is y = αx + β. And r represents the Pearson correlation coefficient. The median and 1σ interval are listed. As we do not apply any uncertainty to our simulations, the resulting 1σ credible intervals are correspondingly narrow.
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