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Table 2.
Physical parameters derived from the hydrodynamic modelling using MCMC methods.
| SN | texp (MJD) | scale | MZAMS (M⊙) | E (foe) | MNi (M⊙) | 56Ni mixing (%) |
|---|---|---|---|---|---|---|
| 2004A | 53009.2 |
0.90 ± 0.04 | 11.43 |
0.51 ± 0.01 | 0.060 |
51 |
| 2004et | 53270.0 |
0.88 |
15.72 |
0.97 ± 0.03 | 0.048 |
50 |
| 2005cs | 53548.6 |
1.36 ± 0.01 | 9.55 ± 0.09 | 0.200 |
0.002 ± 0.0002 | 60 |
| 2008bk | 54539.7 |
0.95 |
9.11 |
0.190 ± 0.003 | 0.008 ± 0.0004 | 74 |
| 2012aw | 56002.8 |
0.99 ± 0.01 | 14.35 |
0.90 ± 0.05 | 0.060 ± 0.001 | 49 |
| 2012ec | 56147.8 |
0.89 |
9.87 |
0.59 ± 0.02 | 0.034 |
28 |
| 2017eaw | 57887.1 |
1.04 ± 0.02 | 15.47 |
1.29 ± 0.03 | 0.079 |
50 ± 2 |
| 2018aoq | 58207.8 |
1.02 |
9.87 |
0.31 ± 0.03 | — | — |
Notes. Results for SN 2004et correspond to d = 5.9 ± 0.4 Mpc. We characterise the results by the median of the posterior distribution and the 16th and 84th percentiles as our lower and upper uncertainties.
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