Open Access

Table A.2.

SNcc yield models used in this work via the abunfit package (see below for references).

Category Name Ref. Remarks
SNcc

Input Ro10_0 a,b Zinit = 0 Z, M[8, 50]M
Ro10_2E-6 a,b Zinit = 0.0001Z, M[8, 50]M
Ro10_2E-4 a,b Zinit = 0.01Z, M[8, 50]M
Ro10_2E-3 a,b Zinit = 0.1Z, M[8, 50]M
Ro10_2E-2 a,b Zinit = 1 Z, M[8, 50]M
Nomoto No13_SNcc_0 c Core-collapse Zinit = 0 Z, M ∈ [11, 140] M
No13_SNcc_0.001 c Core-collapse Zinit = 0.05 Z, M ∈ [11, 40] M
No13_SNcc_0.004 c Core-collapse Zinit = 0.2 Z, M ∈ [11, 40] M
No13_SNcc_0.008 c Core-collapse Zinit = 0.4 Z, M ∈ [11, 40] M
No13_SNcc_0.02 c Core-collapse Zinit = 1 Z, M ∈ [11, 40] M
No13_SNcc_0.05 c Core-collapse Zinit = 2.5 Z, M ∈ [11, 40] M
No13_PISNe_0 c Pair-instability SNeZinit = 0 Z, M ∈ [140, 300] M
No13_SNe_0 c Core-collapse M ∈ [11, 140] M and pair-instability M ∈ [140, 300] M, Zinit = 0 Z
No13_HNe_0 c Hyper-novae Zinit = 0 ZZ, M ∈ [20, 140] M
No13_HNe_0.001 c Hyper-novae Zinit = 0.05 Z, M ∈ [20, 40] M
No13_HNe_0.004 c Hyper-novae Zinit = 0.2 Z, M ∈ [20, 40] M
No13_HNe_0.008 c Hyper-novae Zinit = 0.4 Z, M ∈ [20, 40] M
No13_HNe_0.02 c Hyper-novae Zinit = 1 Z, M ∈ [20, 40] M
No13_HNe_0.05 c Hyper-novae Zinit = 2.5 Z, M ∈ [20, 40] M
Massive He0210_SNcc_0 d,e Core-collapse Zinit = 0 Z, M ∈ [10, 100] M
He0210_PISNe_0 d,e Pair-instability SNeZinit = 0 Z, M ∈ [140, 260] M
He0210_SNe_0 d,e Core-collapse M ∈ [10, 100] M and pair-instability, M ∈ [140, 260] M, Zinit = 0 Z
Neutrino Su16_N20 f Incl. neutrino transport, calibrated for a Nomoto & Hashimoto (1988) progenitor to explode as SN1987A, Zinit = 1 Z, M ∈ [12, 120] M
Su16_W18 f Incl. neutrino transport, calibrated for a Utrobin et al. (2015) progenitor to explode as SN1987A, Zinit = 1 Z, M ∈ [12, 120] M

Notes. Models used in our input cosmological simulations are given in bold.

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