Table 1.
SN Ia explosion models we used.
| Ref. | Model | Mechanism | Model Name | ρc | MWD | MHe | Zprogenitor |
|---|---|---|---|---|---|---|---|
| [used in the present work] | [108 g cm−3] | [M⊙] | [M⊙] | [Z⊙] | |||
| LN18 | Near-Mch | DDT | LN18_100 | 10 | 1.33 | – | |
| LN18_300 | 30 | 1.38 | – | 0, 0.1, 0.5, 1, 2, 3, 5 | |||
| LN18_500 | 50 | 1.39 | – | ||||
| LN20_110-100 | 0.62 | 1.10 | 0.10 | ||||
| LN20 | Sub-Mch | DD | LN20_110-050 | 0.62 | 1.10 | 0.05 | 0, 0.1, 0.5, 1, 2, 3, 5 |
| LN20_100-050 | 0.32 | 1.00 | 0.05 | ||||
| Ref. | Model | Mechanism | Model Name | ρc | Mcore | Mshell | Zprogenitor |
| [used in the present work] | [108 g cm−3] | [M⊙] | [M⊙] | [Z⊙] | |||
| G21_M11_XX | – | 1.1 | 0.05 | ||||
| G21 | Sub-Mch | DD | G21_M10_XX | – | 1.0 | 0.02, 0.03, 0.05, 0.1 | 0.001, 0.1, 1, 3 |
| G21_M09_XX | – | 0.9 | 0.03, 0.05, 0.1 | ||||
| G21_M08_XX | – | 0.8 | 0.03, 0.05, 0.1 | ||||
Notes. “Mechanism” is the SN Ia explosion mechanism: “DDT” means deflagration-to-detonation transition, and “DD” means double-detonation models. “ρc” is the central density of the WD in units of 108 g cm−3. “MWD” and “MHe” represent the total mass of the WD and the helium envelope mass, respectively, in units of M⊙. “Mcore” and “Mshell” indicate the initial core and the initial shell mass of the WD, respectively, in units of M⊙. “Zprogenitor” is the progenitor metallicity in units of Z⊙. “Model Name” is the name of the model we used based on the references. For LN18, we only considered ρc (three digits), such that “100” means ρc = 1.0 × 109 g cm−3. For LN20, the model name consists of MWD (three digits) and MHe (three digits). For G21, the model name is based on the Mcore (two digits) and Mshell (two digits), such that “M10_05” means Mcore = 1.0 M⊙ and Mshell = 0.05 M⊙. We note that a double dash in the table indicates that no information was provided in the reference.
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