Table 4
Estimated physical parameters of our sample of LMC late O-type stars, grouped according to their cluster membership.
VFTS | Classification | Location | Teff | log g | log gc (1) | R⋆ (2) | log Q | v sin i(3) | vr | ɛSi |
---|---|---|---|---|---|---|---|---|---|---|
(kK) | (cm s−2) | (cm s−2) | (R⊙) | (km s−1) | (km s−1) | |||||
346 | O9.7 III | NGC 2070 | 31.4 ± 1.0 | 4.15 ± 0.10 | 4.15 | 6.44 | −12.75 ± 0.20 | 75 | 265 | 7.00 ± 0.20 |
412 | O9.7 | NGC 2070 | 31.0 ± 1.0 | 4.00 ± 0.10 | 4.00 | 5.40 | −12.68 ± 0.2 | 80 | 270 | 7.10 ± 0.10 |
444 | O9.7 | NGC 2070 | 31.0 ± 1.0 | 4.15 ± 0.10 | 4.16 | 7.22 | −12.57 ± 0.2 | 100 | 265 | 7.10 ± 0.10 |
528 | O9.7(n) | NGC 2070 | 30.8 ± 1.0 | 4.15 ± 0.10 | 4.16 | 7.65 | −12.93 ± 0.2 | 150 | 270 | 7.00 ± 0.20 |
569 | O9.2 III: | NGC 2070 | 32.6 ± 1.0 | 3.90 ± 0.10 | 3.90 | 7.49 | −12.74 ± 0.20 | 35 | 255 | 7.00 ± 0.10 |
571 (*) | O9.5 II-III(n) | NGC 2070 | 32.8 ± 2.0 | 4.25 ± 0.10 | 4.26 | 5.46 | <−13.22 | 148 | 260 | 6.90 ± 0.20 |
607 | O9.7 III | NGC 2070 | 32.0 ± 1.0 | 4.10 ± 0.10 | 4.10 | 5.97 | −12.64 ± 0.20 | 60 | 265 | 7.00 ± 0.15 |
615 | O9.5 IIInn | NGC 2070 | 32.0 ± 1.5 | 4.00 ± 0.15 | 4.08 | 10.30 | −12.87 ± 0.20 | 372 | 270 | 7.00 ± 0.20 |
620 | O9.7 III(n) | NGC 2070 | 32.0 ± 1.5 | 4.10 ± 0.15 | 4.15 | 4.82 | −13.15 ± 0.20 | 208 | 275 | 7.00 ± 0.20 |
622 | O9.7 III | NGC 2070 | 32.0 ± 1.0 | 4.20 ± 0.10 | 4.21 | 4.64 | −12.86 ± 0.20 | 84 | 265 | 7.00 ± 0.10 |
070 | O9.7 II | NGC 2060 | 32.0 ± 1.0 | 4.00 ± 0.10 | 4.01 | 5.64 | −13.35 ± 0.15 | 126 | 277 | 7.00 ± 0.20 |
077 | O9.5: IIIn | NGC 2060 | 34.0 ± 1.5 | 4.20 ± 0.15 | 4.24 | 5.20 | < −13.50 | 225 | 275 | 7.10 ± 0.30 |
080 | O9.7 II-III((n)) | NGC 2060 | 32.0 ± 1.5 | 3.85 ± 0.15 | 3.89 | 7.55 | < −13.50 | 190 | 275 | 7.00 ± 0.20 |
091 | O9.5 IIIn | NGC 2060 | 32.0 ± 1.5 | 3.80 ± 0.15 | 3.88 | 7.98 | < −13.50 | 308 | 275 | 7.10 ± 0.30 |
113 | O9.7 II/B0 IV? | NGC 2060 | 32.0 ± 1.0 | 4.25 ± 0.10 | 4.25 | 5.19 | −12.89 ± 0.12 | 35 | 275 | 7.00 ± 0.15 |
128 | O9.5 III:((n)) | NGC 2060 | 33.0 ± 1.0 | 4.15 ± 0.15 | 4.17 | 5.01 | < −13.28 | 180 | 270 | 7.00 ± 0.20 |
131 | O9.7 | NGC 2060 | 32.8 ± 1.0 | 4.38 ± 0.10 | 4.39 | 4.49 | −12.87 ± 0.3 | 124 | 275 | 7.10 ± 0.20 |
141 | O9.5 II-III((n)) | NGC 2060 | 32.3 ± 1.0 | 4.20 ± 0.15 | 4.21 | 8.44 | −12.87 ± 0.20 | 160 | 275 | 7.00 ± 0.20 |
188 (*) | O9.7: III | NGC 2060 | 34.0 ± 2.0 | 4.40 ± 0.10 | 4.40 | 6.42 | −13.22 ± 0.31 | 100 | 275 | 7.00 ± 0.20 |
192 (*) | O9.7 II/B0 IV | NGC 2060 | 31.7 ± 2.0 | 4.13 ± 0.10 | 4.13 | 4.85 | −13.05 ± 0.17 | 40 | 270 | 7.10 ± 0.20 |
205 | O9.7 II((n))/B0 IV((n)) | NGC 2060 | 31.0 ± 1.0 | 4.30 ± 0.15 | 4.31 | 6.29 | < −13.50 | 158 | 265 | 6.90 ± 0.20 |
207 | O9.7 II((n)) | NGC 2060 | 31.4 ± 1.0 | 4.20 ± 0.15 | 4.21 | 5.76 | −13.20 ± 0.3 | 160 | 270 | 7.10 ± 0.20 |
210 | O9.7 II-III((n)) | NGC 2060 | 32.0 ± 1.0 | 4.00 ± 0.15 | 4.02 | 6.47 | −12.78 ± 0.2 | 162 | 275 | 7.10 ± 0.10 |
104 | O9.7 II-III((n)) | Field | 32.0 ± 1.5 | 4.10 ± 0.15 | 4.14 | 5.10 | −13.50 ± 0.30 | 198 | 260 | 7.00 ± 0.20 |
226 | O9.7 III | Field | 33.0 ± 1.0 | 4.20 ± 0.10 | 4.20 | 5.31 | −13.50 ± 0.3 | 64 | 190 | 7.10 ± 0.10 |
328 | O9.5 III(n) | Field | 33.6 ± 1.5 | 4.15 ± 0.15 | 4.19 | 5.12 | < −13.28 | 240 | 300 | 7.00 ± 0.20 |
370 | O9.7 III | Field | 32.0 ± 1.0 | 4.00 ± 0.10 | 4.00 | 5.88 | < −13.47 | 75 | 230 | 7.00 ± 0.15 |
495 | O9.7 II-IIIn | Field | 32.0 ± 1.5 | 4.20 ± 0.15 | 4.22 | 6.44 | −13.50 ± 0.2 | 218 | 270 | 7.00 ± 0.20 |
574 | O9.5 IIIn | Field | 32.0 ± 1.5 | 4.10 ± 0.15 | 4.17 | 5.17 | < −13.38 | 270 | 270 | 6.90 ± 0.20 |
753 | O9.7 II-III | Field | 32.5 ± 1.0 | 4.00 ± 0.10 | 4.00 | 7.74 | < −13.50 | 40 | 270 | 7.20 ± 0.10 |
787 (+) | O9.7 III | Field | 32.8 ± 1.0 | 4.35 ± 0.10 | 4.35 | 5.77 | −12.76 ± 0.2 | 40 | 275 | 7.00 ± 0.20 |
843 | O9.5 IIIn | Field | 32.0 ± 1.5 | 3.90 ± 0.15 | 4.02 | 6.03 | < −13.50 | 318 | 275 | 7.10 ± 0.30 |
Notes. In addition to standard abbreviations, log gc is the centrifugally corrected surface gravity. Estimates of log Q were derived assuming unclumped winds and β = 0.9. For all objects, YHe = 0.1 ± 0.02 was found. Uncertainties in our v sin i estimates range from 10 to ~20%, with higher values typical for more rapid rotators. (1) log gc = log[g + (v sin i)2 /R⋆], see e.g. Repolust et al. (2004); (2)adopted from RA17; (3)italicised values differ from those from RA17 by more than 1σ; (*) objects with asymmetric and blueshifted He II λ4686; (+) macroturblence of vmac = 45 km s−1 was needed to reproduce the observed line profiles.
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