Table 9.
Summary of PISN model parameters.
| Name | M(ZAMS) | M(He) | M(Ni) | Metallicity | vejecta | Ekin |
|---|---|---|---|---|---|---|
| (M⊙) | (M⊙) | (M⊙) | (Z/Z⊙) | (km s−1) | (1051 erg) | |
| He100 | 205 | 100 | 6 | 0.01 | 8400 | 42 |
| He120 | 242 | 120 | 26 | 0.01 | 10 000 | 71 |
| He125 | 251 | 125 | 34 | 0.01 | 10 300 | 79 |
| He130 | 260 | 130 | 44 | 0.01 | 10 600 | 87 |
| P250Ni25 | 250 | 127 | 25 | 0.07 | 7500 | 82 |
| P250Ni34 | 250 | 127 | 34 | 0.07 | 8850 | 82 |
Notes. The mass in column (3) lists the mass of the He core before the progenitor explodes. The values of the He100–He130 models were taken from https://2sn.org/DATA/HW01/bulk_yields.txt and are based on Heger & Woosley (2002). The values of the P250 models are from Kozyreva et al. (2017) and Gilmer et al. (2017). The ZAMS masses of the He100–He130 models are computed with M(He)=13/24 × [M(ZAMS)−20 M⊙] (Heger & Woosley 2002).
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