Open Access
Table 1.
Evolutionary parameters for Pop III SMS models.
| Start of H burning | End of H burning | |||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| Mass | v/vcrit | Lifetime | tblue | tred | Mcc | veq | Ltot | ΓEdd | Mcc | veq | Ltot | ΓEdd |
| (M⊙) | (Myr) | (Myr) | (Myr) | (km s−1) | (1053 g cm2 s−1) | (km s−1) | (1053 g cm2 s−1) | |||||
| 1000 | 0.01 | 1.658 | 1.637 | 0.000 | 0.942 | 26.600 | 5.108 | 0.793 | 0.510 | 7.360 | 4.930 | 0.883 |
| 2000 | 0.01 | 1.442 | 1.426 | 0.000 | 0.952 | 31.400 | 16.040 | 0.865 | 0.510 | 2.360 | 16.044 | 0.923 |
| 3000 | 0.01 | 1.350 | 1.335 | 0.000 | 0.955 | 34.500 | 31.402 | 0.898 | 0.506 | 9.950 | 30.754 | 0.942 |
| 4000 | 0.01 | 1.286 | 1.273 | 0.000 | 0.955 | 36.700 | 49.478 | 0.917 | 0.520 | 14.800 | 46.923 | 0.950 |
| 5000 | 0.01 | 1.175 | 1.106 | 0.056 | 0.957 | 38.700 | 71.264 | 0.930 | 0.564 | 3.000 | 66.299 | 0.962 |
| 6000 | 0.01 | 1.168 | 1.086 | 0.070 | 0.958 | 40.400 | 96.316 | 0.940 | 0.608 | 3.000 | 80.615 | 0.954 |
| 7000 | 0.01 | 1.164 | 1.043 | 0.109 | 0.959 | 41.800 | 122.912 | 0.947 | 0.480 | 3.000 | 108.858 | 0.946 |
| 8000 | 0.01 | 1.117 | 1.001 | 0.104 | 0.959 | 41.000 | 132.190 | 0.953 | 0.568 | 0.144 | 119.633 | 0.962 |
| 9000 | 0.01 | 1.143 | 1.099 | 0.037 | 0.958 | 44.100 | 177.906 | 0.959 | 0.511 | 0.146 | 175.794 | 0.971 |
| 10 000 | 0.01 | 1.028 | 0.901 | 0.121 | 0.957 | 45.100 | 209.965 | 0.963 | 0.640 | 0.305 | 162.181 | 0.957 |
| 1000 | 0.05 | 1.741 | 1.720 | 0.000 | 0.941 | 134.000 | 25.691 | 0.793 | 0.522 | 25.600 | 25.671 | 0.896 |
| 2000 | 0.05 | 1.463 | 1.447 | 0.000 | 0.950 | 158.000 | 80.666 | 0.865 | 0.524 | 24.100 | 80.759 | 0.926 |
| 3000 | 0.05 | 1.348 | 1.334 | 0.000 | 0.954 | 174.000 | 158.032 | 0.897 | 0.527 | 0.311 | 158.876 | 0.942 |
| 4000 | 0.05 | 1.286 | 1.273 | 0.000 | 0.954 | 184.000 | 248.373 | 0.916 | 0.543 | 0.000 | 249.705 | 0.953 |
| 5000 | 0.05 | 1.260 | 1.247 | 0.000 | 0.955 | 194.000 | 357.462 | 0.929 | 0.530 | 2.100 | 359.237 | 0.961 |
| 6000 | 0.05 | 1.227 | 1.158 | 0.058 | 0.957 | 203.000 | 485.122 | 0.939 | 0.571 | 0.991 | 446.133 | 0.970 |
| 7000 | 0.05 | 1.204 | 1.177 | 0.015 | 0.956 | 210.000 | 617.091 | 0.947 | 0.572 | 1.870 | 619.190 | 0.970 |
| 8000 | 0.05 | 1.178 | 1.166 | 0.000 | 0.958 | 206.000 | 658.331 | 0.953 | 0.575 | 0.001 | 662.250 | 0.970 |
| 9000 | 0.05 | 1.158 | 0.977 | 0.013 | 0.959 | 230.000 | 970.288 | 0.958 | 0.646 | 0.000 | 975.517 | 0.971 |
| 10 000 | 0.05 | 1.070 | 0.901 | 0.103 | 0.967 | 179.000 | 940.312 | 0.960 | 0.709 | 1.720 | 792.292 | 0.963 |
| 1000 | 0.10 | 1.848 | 1.768 | 0.059 | 0.939 | 268.000 | 51.182 | 0.791 | 0.523 | 28.005 | 46.985 | 0.906 |
| 2000 | 0.10 | 1.505 | 1.440 | 0.058 | 0.947 | 315.000 | 160.639 | 0.863 | 0.556 | 0.748 | 127.237 | 0.937 |
| 3000 | 0.10 | 1.413 | 1.266 | 0.133 | 0.950 | 347.000 | 314.233 | 0.895 | 0.613 | 0.768 | 261.266 | 0.949 |
| 4000 | 0.10 | 1.322 | 1.202 | 0.107 | 0.952 | 368.000 | 492.497 | 0.915 | 0.671 | 1.110 | 390.916 | 0.958 |
| 5000 | 0.10 | 1.300 | 1.285 | 0.002 | 0.954 | 383.000 | 705.955 | 0.928 | 0.550 | 2.802 | 591.312 | 0.965 |
| 6000 | 0.10 | 1.315 | 1.163 | 0.139 | 0.954 | 406.000 | 961.128 | 0.937 | 0.051 | 0.014 | 779.156 | 0.947 |
| 7000 | 0.10 | 1.236 | 1.094 | 0.129 | 0.954 | 420.000 | 1225.720 | 0.945 | 0.243 | 1.550 | 1035.676 | 0.951 |
| 8000 | 0.10 | 1.270 | 1.123 | 0.135 | 0.955 | 434.000 | 1511.272 | 0.951 | 0.619 | 1.550 | 1289.506 | 0.971 |
| 9000 | 0.10 | 1.227 | 1.097 | 0.122 | 0.956 | 448.000 | 1817.557 | 0.956 | 0.657 | 3.370 | 1530.294 | 0.965 |
| 10 000 | 0.10 | 1.148 | 0.975 | 0.178 | 0.955 | 449.000 | 2084.810 | 0.961 | 0.710 | 5.460 | 1765.897 | 0.965 |
Notes. The lifetime and cumulative time in red (log Teff ≤ 4.00) and blue (log Teff > 4.00) phases; core mass fraction Mcc, equatorial velocity veq, total angular momentum Ltot, and Eddington factor ΓEdd at the start and end of H burning.
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