Table D.1
Optimal parameters of the Nuker model used to fit the CO integrated emission of several sources from the full Lupus sample, based on the criteria described in Appendix C.
| # | Object | ρt | γ | β | α | Ftot | ρend |
|---|---|---|---|---|---|---|---|
| [′′] | [–] | [–] | [–] | [mJy beam−1] | [′′] | ||
| 1 | EXLup | 1.20 ± 0.15 | − 0.09 ± 0.01 | 6.86 ± 0.63 | 1.23 ± 0.04 | 296 ± 1 | 1.4 |
| 2 | RYLup | 0.37 ± 0.01 | − 0.01 ± 0.01 | 2.38 ± 0.05 | 2.25 ± 0.08 | 952 ± 9 | 2.7 |
| 3 | Sz75 | 0.58 ± 0.02 | 0.10 ± 0.01 | 2.83 ± 0.10 | 2.61 ± 0.09 | 448 ± 3 | 1.9 |
| 4 | Sz82 | 6.93 ± 1.42 | − 0.10 ± 0.01 | 6.21 ± 0.74 | 0.93 ± 0.03 | 2824 ± 14 | 8.2 |
| 5 | Sz83 | 0.20 ± 0.01 | 0.01 ± 0.01 | 1.58 ± 0.02 | 2.33 ± 0.11 | 748 ± 7 | 2.6 |
| 6 | Sz91 | 0.38 ± 0.01 | 0.01 ± 0.01 | 1.99 ± 0.04 | 2.00 ± 0.07 | 268 ± 2 | 2.5 |
| 7 | Sz111 | 0.22 ± 0.01 | 0.06 ± 0.01 | 1.23 ± 0.01 | 6.49 ± 0.44 | 598 ± 4 | 3.2 |
| 8 | V1192Sco | 0.31 ± 0.01 | − 0.14 ± 0.01 | 1.96 ± 0.05 | 3.42 ± 0.21 | 141 ± 1 | 1.8 |
| 9 | SSTc2d J160703.9-391112 | 0.71 ± 0.01 | 0.07 ± 0.01 | 2.38 ± 0.08 | 10.00 ± 1.33 | 139 ± 1 | 1.7 |
| 10 | SSTc2d J160830.7-382827 | 0.53 ± 0.01 | − 0.07 ± 0.01 | 2.22 ± 0.02 | 3.03 ± 0.06 | 1187 ± 4 | 2.7 |
Notes. The modeling of the integrated line emission is performed following the methodology from Sect. 3.1. The parameters of the Nuker function are: the transition radius ρt , the inner and outer slopes γ and β, the smoothing parameter α, and the integrated total flux Ftot. An additional parameter ρend was used as the outermost radius of the Nuker model, which is set to coincide with the radial distance at which the azimuthally averaged line emission reaches a zero value.
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