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Prog. | SN | Rem. |
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Prog. | SN | Rem. |
Z = 0.004 | Z = 0.020 | ||||||||||||||
12 | 11.8 | 3.74 | 1.78 | 1.4 | SG | II | NS | 12 | 10.5 | 3.81 | 1.94 | 1.4 | SG | II | NS |
15 | 14.1 | 5.01 | 2.84 | 1.7 | SG | II | NS | 15 | 10.2 | 5.97 | 3.61 | 1.7 | SG | II | NS |
20 | 18.0 | 7.45 | 4.79 | 2.0 | SG | II | NS | 20 | 11.8 | 9.01 | 6.62 | 2.0 | SG | II | NS |
25 | 20.0 | 9.95 | 7.06 | 2.5 | SG | II | NS | 25 | 11.3 | 11.33 | 8.98 | 2.5 | WNL | II | NS |
30 | 18.9 | 14.16 | 11.14 | 2.9 | SG | II | BH | 40 | 12.7 | 12.70 | 11.75 | 3.0 | WC | Ic | BH |
40 | 22.3 | 21.59 | 17.16 | 3.5 | WNL | II | BH | 60 | 14.6 | 14.60 | 13.67 | 3.6 | WC | Ic | BH |
60 | 28.5 | 28.50 | 28.46 | 4.4 | WO | Ic | BH | 85 | 12.3 | 12.30 | 11.22 | 3.0 | WC | Ic | BH |
120 | 17.2 | 17.20 | 17.18 | 3.4 | WC | Ic | BH | 120 | 11.3 | 11.30 | 10.40 | 2.8 | WC | Ic | BH |
Z = 0.008 | Z = 0.040 | ||||||||||||||
201 | 15.5 | - | 4.85 | 2.1 | SG | II | NS | 20 | 9.2 | 9.05 | 6.84 | 1.4 | SG | II | NS |
251 | 14.0 | - | 6.92 | 2.7 | SG | II | NS | 25 | 9.6 | 9.60 | 8.19 | 1.7 | WC | Ib | NS |
30 | 12.1 | 12.10 | 11.10 | 2.9 | WC | Ic | BH | 40 | 11.4 | 11.40 | 10.48 | 2.8 | WC | Ic | BH |
40 | 17.4 | 17.40 | 17.23 | 3.5 | WC | Ic | BH | 85 | 7.2 | 7.20 | 6.07 | 2.2 | WC | Ic | NS |
60 | 16.4 | 16.40 | 16.44 | 3.3 | WO | Ic | BH | 120 | 7.1 | 7.10 | 6.10 | 2.2 | WC | Ic | NS |
120 | 13.4 | 13.40 | 13.24 | 3.0 | WC | Ic | BH | ||||||||
Homogenous model at Z = 0.002 | |||||||||||||||
602 | 27.8 | - | - | 4.0 | WC | Ib | BH |
(1) Non-rotating models from Meynet et al. (1994) used to estimate the minimum initial mass of stars ending their lifetime
in the WNL phase at that metallicity. These models were computed with artificially enhanced mass loss rates, which
somewhat compensates for the neglect of the effects of rotation.
(2) Model computed up to the end of silicon burning.
Note: All masses are given in
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