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Table 1.

Ejecta model properties.

Model MpreSN Mej Ekin Vm 4He 12C 14N 16O 24Mg 28Si 40Ca 56Nit = 0 V max , 56 N i $ V_{\mathrm{max},{{\ensuremath{^{56}\rm{N}}}i}} $
[M] [M] [foe] [km s−1] [M] [M] [M] [M] [M] [M] [M] [M] [km s−1]
he3p30 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) 3712
he6p00 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) 4990
he8p00 5.63 3.95 0.71 4251 0.84 0.49 5.17(–3) 1.71 1.10(–1) 4.89(–2) 2.00(–3) 5.46(–2) 3435
he12p00 7.24 5.32 0.81 3911 0.23 1.00 1.42(–4) 3.03 8.73(–2) 7.41(–2) 3.42(–3) 7.90(–2) 2531

Notes. The table columns correspond to the preSN mass, the ejecta mass, the ejecta kinetic energy (1 foe ≡1051 erg), the mean expansion rate V m 2 E kin / M ej $ V_{\mathrm{m}} \equiv \sqrt{2E_{\mathrm{kin}}/M_{\mathrm{ej}}} $, the cumulative yields of 4He, 12C, 14N, 16O, 24Mg, 28Si, 40Ca, and 56Ni prior to decay, as well as the ejecta velocity that bounds 99% of the total 56Ni mass in the corresponding model. Numbers in parenthesis correspond to powers of ten.

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