Table 1
Ejecta properties for our set of explosion models.
| Model | MZAMS (M⊙) | MpreSN (M⊙) | Mej (M⊙) | Ekin [foe] | Vm [km s−1] | 4He (M⊙) | 12C (M⊙) | 14N (M⊙) | 16O (M⊙) | 24Mg (M⊙) | 28Si (M⊙) | 40Ca (M⊙) | 56Nit=o (M⊙) | 58Ni (M⊙) |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| he2p6 | 13.85 | 2.15 | 0.79 | 0.13 | 4134 | 0.71 | 0.02 | 4.78(−3) | 2.28(−2) | 1.58(−3) | 3.35(−3) | 2.40(−4) | 1.22(−2) | 1.53(−3) |
| he2p9 | 14.82 | 2.37 | 0.93 | 0.37 | 6336 | 0.77 | 0.04 | 5.15(−3) | 5.03(−2) | 3.82(−3) | 1.01(−2) | 5.62(−4) | 2.32(−2) | 1.48(−3) |
| he3p3 | 16.07 | 2.67 | 1.20 | 0.55 | 6777 | 0.84 | 0.06 | 6.21(−3) | 1.51(−1) | 1.75(−2) | 2.76(−2) | 1.00(−3) | 4.00(−2) | 3.61(−3) |
| he3p5 | 16.67 | 2.81 | 1.27 | 0.41 | 5704 | 0.87 | 0.07 | 6.31(−3) | 1.72(−1) | 1.60(−2) | 2.13(−2) | 7.34(−4) | 2.92(−2) | 2.43(−3) |
| he4p0 | 18.11 | 3.16 | 1.62 | 0.63 | 6272 | 0.92 | 0.10 | 6.46(−3) | 3.10(−1) | 2.98(−2) | 4.70(−2) | 1.35(−3) | 4.45(−2) | 3.47(−3) |
| he4p5 | 19.50 | 3.49 | 1.89 | 1.17 | 7884 | 0.95 | 0.13 | 6.52(−3) | 4.19(−1) | 3.73(−2) | 6.14(−2) | 2.40(−3) | 8.59(−2) | 6.09(−3) |
| he5p0 | 20.82 | 3.81 | 2.21 | 1.51 | 8286 | 0.97 | 0.15 | 6.60(−3) | 5.92(−1) | 5.20(−2) | 5.55(−2) | 2.26(−3) | 9.77(−2) | 7.56(−3) |
| he6p0 | 23.33 | 4.44 | 2.82 | 1.10 | 6269 | 0.95 | 0.25 | 6.20(−3) | 9.74(−1) | 1.01(−1) | 5.88(−2) | 2.12(−3) | 7.04(−2) | 5.00(−3) |
| he7p0 | 25.68 | 5.04 | 3.33 | 1.38 | 6456 | 0.90 | 0.39 | 5.42(−3) | 1.29(0) | 1.07(−1) | 9.47(−2) | 3.42(−3) | 1.02(−1) | 4.19(−3) |
| he8p0 | 27.91 | 5.63 | 3.95 | 0.71 | 4251 | 0.84 | 0.49 | 5.17(−3) | 1.71(0) | 1.10(−1) | 4.89(−2) | 2.00(−3) | 5.46(−2) | 3.46(−3) |
| he12p0 | 35.74 | 7.24 | 5.32 | 0.81 | 3911 | 0.23 | 1.00 | 1.42(−4) | 3.03(0) | 8.73(−2) | 7.41(−2) | 3.42(−3) | 7.90(−2) | 2.47(−3) |
| he2p5MdZ | 13.51 | 2.5 | 1.10 | 0.43 | 6237 | 0.87 | 0.05 | 4.08(−3) | 9.20(−2) | 3.41(−3) | 1.33(−2) | 8.39(−4) | 3.48(−2) | 2.58(−3) |
| he3p0MdZ | 15.14 | 3.0 | 1.45 | 0.72 | 7077 | 0.98 | 0.08 | 7.12(−3) | 2.07(−1) | 1.29(−2) | 3.82(−2) | 2.25(−3) | 5.64(−2) | 2.51(−3) |
| he3p5MdZ | 16.67 | 3.5 | 1.93 | 1.21 | 7941 | 1.06 | 0.10 | 7.34(−3) | 4.26(−1) | 4.25(−2) | 7.14(−2) | 3.57(−3) | 1.02(−1) | 5.02(−3) |
| he4p0MdZ | 18.11 | 4.0 | 2.34 | 1.20 | 7168 | 1.11 | 0.13 | 7.45(−3) | 6.71(−1) | 5.88(−2) | 8.93(−2) | 4.53(−3) | 1.07(−1) | 4.75(−3) |
| he4p5MdZ | 19.50 | 4.5 | 2.78 | 1.20 | 6573 | 1.15 | 0.16 | 6.60(−3) | 9.62(−1) | 7.91(−2) | 9.27(−2) | 4.33(−3) | 1.01(−1) | 4.44(−3) |
Notes. The upper part describes the models already used in D21 while the lower part describes new models arising from progenitors evolved without wind mass loss. The table columns correspond to the ZAMS mass, the preSN mass, the ejecta mass, the ejecta kinetic energy (1 foe ≡ 1051 erg), the mean expansion rate 
, the cumulative yields of 4He, 12C, 14N, 16O, 24Mg, 28Si, 40Ca, 56Ni prior to decay, and 58Ni. All 56Ni masses used here were taken from the KEPLER approximation to the P-HOTB neutrino simulation (see discussion in D21).
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