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Table 1.

Dependence of pre-SN properties on physical parameters.

M He i Mathematical equation: $ M_{\mathrm{He}}^{\mathrm{i}} $ Z fov MCO XC MC-free ξ2.5 μ4 M4 sc MFe Mf log( − Ebind) Eexp Fate Mrm, grav
[M] [M] [M] [NAkB] [M] [M] [erg] [1051erg] [M]
15.0 0.0088 0.01 9.25 0.247 1.92 0.145 0.05 1.67 0.87 1.56 11.5 51.49 0.24 NS 1.46
15.0 0.02 0.01 7.51 0.254 3.28 0.571 0.16 2.32 1.14 1.85 8.79 51.70 BH 8.79
15.0 0.03 0.01 6.45 0.259 2.07 0.163 0.07 1.77 0.92 1.54 7.82 51.58 0.56 NS 1.54
15.0 0.04 0.01 5.81 0.262 2.16 0.189 0.08 1.82 0.95 1.60 7.14 51.56 0.77 NS 1.58

15.0 0.02 0.0 7.70 0.253 3.35 0.597 0.17 2.37 1.13 1.89 8.96 51.72 BH 8.96
15.0 0.02 0.016 7.43 0.255 3.07 0.535 0.15 2.29 1.12 1.85 8.70 51.67 BH 8.70
15.0 0.02 0.027 7.34 0.256 2.67 0.444 0.13 2.14 1.08 1.79 8.57 51.61 BH 8.57

Notes. Same as Table A.1, but for the representative model M He i = 15 M Mathematical equation: $ M_{\mathrm{He}}^{\mathrm{i}}=15 \, M_{\odot} $, with variations in the physical parameters. We used different metallicities, Z = 0.0088, 0.02, 0.03, 0.04, and explored a range of convective overshooting parameters, fov = 0.0, 0.01, 0.016, 0.027. The case with Z = 0.02 and fov = 0.01 serves as the fiducial model.

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