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Table 2.
Properties of different SMS models considered for the analysis (adopted from Martins et al. 2020).
| ID | Teff | log L | log g | M | R | MF555W |
|---|---|---|---|---|---|---|
| [K] | [L⊙] | [M⊙] | [R⊙] | |||
| A1 | 7000 | 8.0 | 0.5 | 5395 | 6723 | −13.6 |
| A2 | 7000 | 9.0 | 0.5 | 53 956 | 21 506 | −13.6 |
| A3 | 10 000 | 8.0 | 0.8 | 2585 | 3340 | −13.2 |
| A4 | 10 000 | 9.0 | 0.8 | 25 848 | 10 580 | −13.4 |
| B1 | 137 000 | 8.4 | 5.5 | 10 000 | 30 | −6.4 |
| B2 | 43 000 | 8.4 | 3.5 | 10 000 | 301 | −9.6 |
| B3 | 13 600 | 8.4 | 1.5 | 10 000 | 3006 | −13.1 |
| C1 | 77 000 | 7.4 | 4.5 | 1000 | 30 | −8.3 |
| C2 | 43 000 | 7.4 | 3.5 | 1000 | 95 | −9.8 |
| C3 | 24 000 | 7.4 | 2.5 | 1000 | 305 | −11.3 |
Notes. The final column represents the absolute AB magnitude in the F555W band for those SMSs whose mass is rescaled to 103 M⊙ (assuming L ∝ M).
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