Table 2.
Summary of ejecta properties used as initial conditions for our CMFGEN simulations.
| Model | Mej | Ekin | M(56Ni) | M(H) | V99, H | V99, He | V99,56Ni | Xs(H) | Xs(He) |
|---|---|---|---|---|---|---|---|---|---|
| [M⊙] | [1051 erg] | [0.01 M⊙] | [M⊙] | [1000 km s−1] | [1000 km s−1] | [1000 km s−1] | |||
| logP2p75 | 1.90 | 1.02 | 8.97 | 0.00 | ... | 1.79 | 6.47 | 0. | 0.98 |
| logP2p80 | 2.25 | 1.07 | 8.96 | 0.02 | 7.12 | 2.10 | 6.74 | 0.13 | 0.86 |
| logP2p85 | 2.43 | 1.17 | 8.81 | 0.06 | 6.43 | 2.06 | 6.73 | 0.33 | 0.65 |
| logP2p90 | 2.49 | 1.15 | 8.79 | 0.12 | 5.93 | 2.31 | 7.05 | 0.48 | 0.51 |
| logP2p95 | 2.56 | 1.17 | 8.78 | 0.15 | 5.85 | 2.00 | 6.86 | 0.53 | 0.46 |
| logP3p00 | 2.75 | 1.09 | 8.76 | 0.22 | 4.96 | 2.39 | 6.76 | 0.57 | 0.42 |
| logP3p10 | 3.03 | 1.13 | 8.57 | 0.37 | 4.37 | 1.92 | 6.21 | 0.62 | 0.37 |
| logP3p20 | 3.72 | 1.19 | 8.55 | 0.80 | 2.92 | 2.13 | 6.54 | 0.66 | 0.33 |
| logP3p35 | 6.49 | 0.98 | 8.76 | 2.68 | 1.57 | 1.39 | 5.70 | 0.68 | 0.30 |
| logP3p45 | 9.45 | 1.09 | 8.84 | 4.64 | 0.78 | 0.64 | 5.45 | 0.68 | 0.30 |
Notes. The columns give in turn the ejecta mass, the kinetic energy, the 56Ni mass, the hydrogen mass, the velocity bounding 99% of the mass of H, He, and 56Ni (integral performed inwards for H and He and outwards for 56Ni), and the mass fractions of H and He in the outermost ejecta layer. These abundance values slightly differ from those shown in Table 1 because of the adopted chemical mixing (see discussion in Sect. 2.2).
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