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Table 3
Slope α of the power laws fitted to the IMF (Fig. 7) and star-to-BD number ratio for different regions.
| Slope of the IMF (α) | Star-to-BD ratio | Reference | Surface densityd | FFUV,median | |||
|---|---|---|---|---|---|---|---|
| <1 M⊙ | <0.2 M⊙ | 0.03–1 M⊙ | 0.02–1 M⊙ | (pc−2) | (G0) | ||
| CrA | 0.95 ± 0.06 | 0.63 ± 0.14 | ![]() |
![]() |
This worka | 120 | 13.0 |
| Cha I | 0.62 ± 0.13 | 0.67 ± 0.23 | 3.2–4.8 | 2.6–3.7 | Mužic´ et al. (2015)b | 29 | 1.2 |
| Lupus 3 | 0.98 ± 0.38 | 0.29 ± 0.22 | 2.1–4.5 | 2.0–4.0 | Mužic´ et al. (2015)b | 24 | 0.6 |
| NGC 1333 | 0.61 ± 0.08 | 0.48 ± 0.15 | 1.8–2.8 | 1.8–2.7 | Scholz et al. (2012b) | 200 | 27.1 |
| NGC 2244 | 0.98 ± 0.04 | 1.09 ± 0.14 | 2.34 ± 0.25 | 1.74 ± 0.28 | Mužic´ et al. (2019)c | 33 | 11569.8 |
| RCW 38 | 0.91 ± 0.11 | 0.51 ± 0.15 | 2.0 ± 0.6 | Mužic´ et al. (2017) | 3620 | 266124.6 | |
Notes. (a) the mean of the results from the three isochrones; (b) updated as described in Appendix C; (c) values for isochrone 1 and distance of 1400 pc; (d) values from Mužic´ et al. (2019) and Appendix D.
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