Table 3
Some global properties of mixing in the ejecta.
| Model |
|
|
|
Mmix | δ MH | ⟨ X ⟩ |
| (km s-1) | (M⊙) | |||||
|
|
||||||
| B15-1 | 921 | 3103 | 3241 | 11.45 | 0.111 | 0.040 |
| B15-2 | 1222 | 3355 | 3490 | 11.20 | 0.172 | 0.062 |
| B15-3 | 1807 | 4977 | 5678 | 12.31 | 0.329 | 0.118 |
| N20-P | 924 | 1635 | 1790 | 4.80 | 0.262 | 0.039 |
| N20-C | 930 | 1642 | 1797 | 4.79 | 0.375 | 0.052 |
| W18 | 877 | 1395 | 1472 | 4.10 | 0.062 | 0.011 |
| W20 | 783 | 1374 | 1482 | 5.32 | 0.083 | 0.012 |
Notes. The left column gives the name of the hydrodynamic model. is the weighted mean velocity of the bulk mass of 56Ni with the 56Ni mass fraction as weight function; , the maximum velocity of the bulk mass of 56Ni; , the weighted mean velocity of the fast moving 56Ni tail with the 56Ni mass fraction as weight function; Mmix, the mass coordinate out to which the bulk mass of 56Ni is mixed; δMH, the mass of hydrogen mixed into the He shell; and ⟨ X ⟩ is the average mass fraction of hydrogen in the mass shell defined by 
, where MCC and 
are the mass coordinates given in Tables 2 and 1, respectively.
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