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Table 1.

Ejecta properties of our set of Type Ibc models from D21.

Model MZAMS MpreSN Mej Ekin 4He 16O 56Nit = 0
[M] [M] [M] [foe] [M] [M] [M]
he2p6 13.85 2.15 0.79 0.13 0.71 2.28(−2) 1.22(−2)
he2p9 14.82 2.37 0.93 0.37 0.77 5.03(−2) 2.32(−2)
he3p3 16.07 2.67 1.20 0.55 0.84 1.51(−1) 4.00(−2)
he3p5 16.67 2.81 1.27 0.41 0.87 1.72(−1) 2.92(−2)
he4p0 18.11 3.16 1.62 0.63 0.92 3.10(−1) 4.45(−2)
he4p5 19.50 3.49 1.89 1.17 0.95 4.19(−1) 8.59(−2)
he5p0 20.82 3.81 2.21 1.51 0.97 5.92(−1) 9.77(−2)
he6p0 23.33 4.44 2.82 1.10 0.95 9.74(−1) 7.04(−2)
he7p0 25.68 5.04 3.33 1.38 0.90 1.29(0) 1.02(−1)
he8p0 27.91 5.63 3.95 0.71 0.84 1.71(0) 5.46(−2)
he12p0 35.74 7.24 5.32 0.81 0.23 3.03(0) 7.90(−2)

Notes. The table columns correspond to the ZAMS mass, the preSN mass, the ejecta mass, the ejecta kinetic energy (1 foe ≡ 1051 erg), and the cumulative yields of 4He, 16O, and 56Ni prior to decay (see discussion in D21). Numbers in parentheses represent powers of ten.

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