Table 2.
Relevant properties of the hydrodynamic simulations from Jones et al. (2016a).
| Id | Res | CCs |  |
Mrem | Mej | ⟨Ye⟩ | XIGE |
|---|---|---|---|---|---|---|---|
| (g cm−3) | (M⊙) | (M⊙) | |||||
| G13 | 2563 | N | 9.90 | 0.647 | 0.741 | 0.491 | 0.267 |
| G14 | 5123 | N | 9.90 | 0.438 | 0.951 | 0.491 | 0.263 |
| G15 | 2563 | Y | 9.90 | 1.212 | 0.177 | 0.493 | 0.184 |
| J01 | 2563 | N | 9.95 | 0.631 | 0.768 | 0.491 | 0.271 |
| J02 | 2563 | Y | 9.95 | 1.291 | 0.104 | 0.493 | 0.175 |
| J07 | 5763 | N | 9.95 | 0.366 | 1.027 | 0.489 | 0.293 |
Notes. Only the models that are tECSNe are shown. In order from left to right, the columns are: model id, grid resolution, Coulomb corrections included in EoS (Y/N), central density at ignition of the deflagration, bound ONeFe remnant mass, mass of the ejected material, average electron fraction in the ONeFe remnant, and mass fraction of iron-group elements in the ONeFe remnant. The model J07 is a new addition. Nucleosynthesis simulations have been performed for models G14 and J07, which were used for this work.
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