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Table 2

Properties of ejecta models produced from the set of progenitor models presented in Sect. 2.1 and Table 1.

Model Mej Ekin Vm 56Ni0 Epm
[M] [1051 erg] [km s−1] [M] [1049 erg]
he4 1.49 0.75 7117 0.08
he5 2.01 1.02 7134 0.08
he6 2.37 1.21 7152 0.08
he7 2.85 1.46 7187 0.08
he8 3.31 1.67 7135 0.08
he9 3.59 1.81 7119 0.08
he10 3.39 1.77 7239 0.08
he11 3.56 1.77 7068 0.08
he12 3.67 2.11 7608 0.08

he4 1.49 0.75 7117 0.08
he4epl 1.49 1.63 10 504 0.08
he4ep 1.49 1.64 10 509 0.16

he4pml 1.49 0.75 7118 0.08 1.0
he4pmu 1.49 0.75 7124 0.08 2.0

he9 3.59 1.81 7119 0.08
he9pml 3.59 1.81 7121 0.08 1.0
he9pmu 3.59 1.81 7123 0.08 2.0

he12 3.67 2.11 7608 0.08
he12epl 3.68 4.77 11 414 0.08
he12ep 3.69 4.76 11 396 0.16

he12pml 3.67 2.11 7604 0.08 1.0
he12pmu 3.67 2.11 7605 0.08 2.0
he12eppml 3.68 4.76 11 409 0.16 1.0

Notes. For models with a suffix pml and pmu, the magnetar field is 1015 G.

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