Table 2.
Properties of pre-supernova models.
Models | 15 M⊙ | 20 M⊙ | 25 M⊙ | |||
---|---|---|---|---|---|---|
GENEC | MESA | GENEC | MESA | GENEC | MESA | |
Mtot [M⊙] | 13.29 | 11.47 | 18.50 | 17.32 | 17.31 | 19.95 |
log(Rtot/R⊙) | 2.80 | 3.02 | 2.91 | 3.08 | 3.00 | 3.15 |
log(L/L⊙) | 4.88 | 5.02 | 5.21 | 5.28 | 5.41 | 5.43 |
log(Teff [K]) | 3.55 | 3.51 | 3.58 | 3.54 | 3.61 | 3.56 |
MHe, shell [M⊙] | 4.12 | 4.87 | 6.65 | 7.20 | 8.85 | 9.39 |
MCO, shell [M⊙] | 2.29 | 3.12 | 4.30 | 5.10 | 6.38 | 6.97 |
MSi, shell [M⊙] | 1.83 | 1.60 | NA | 1.88 | 2.19 | 2.30 |
MFe, core [M⊙] | 1.65 | 1.49 | 1.87 | 1.71 | 1.84 | 1.82 |
fSi, O | 0.0848 | 0.400 | 0.379 | 0.338 | 0.247 | 0.0493 |
Ye, c | 0.446 | 0.427 | 0.447 | 0.444 | 0.451 | 0.453 |
Ye, core | 0.463 | 0.458 | 0.467 | 0.467 | 0.466 | 0.470 |
MCh [M⊙] | 1.18 | 1.15 | 1.19 | 1.22 | 1.22 | 1.24 |
MFe, deg [M⊙] | 1.31 | 1.31 | 1.30 | 1.39 | 1.30 | 1.39 |
Ψc | 7.92 | 10.4 | 6.86 | 7.87 | 6.53 | 6.87 |
sc [kb/baryon] | 0.872 | 0.749 | 0.907 | 0.936 | 0.943 | 1.05 |
log(ρc [g cm−3]) | 9.65 | 10.2 | 9.42 | 9.78 | 9.36 | 9.59 |
log(Tc [K]) | 9.92 | 10.0 | 9.90 | 9.97 | 9.90 | 9.96 |
ξMr = 2.5 | 0.0375 | 0.128 | 0.267 | 0.240 | 0.289 | 0.422 |
ξs = 4 | 0.671 | 0.712 | 0.493 | 0.750 | 0.651 | 0.589 |
M4 [M⊙] | 1.67 | 1.57 | 1.87 | 1.87 | 1.84 | 2.29 |
μ4 | 0.0126 | 0.0888 | 0.158 | 0.129 | 0.154 | 0.130 |
M4, g | 1.49 | 1.41 | 1.65 | 1.62 | 1.65 | 1.97 |
Notes. Mtot is the total mass of the star, Rtot the total radius, L the luminosity at the surface and Teff the surface effective temperature. The shell masses correspond to the outer mass coordinate where the element in question is most abundant; NA is used if at no point in the star is that species the most abundant. fSi, O is as defined in Eq. (22). The thermodynamic variables ρ, s, Ye, and T evaluated at the innermost point of the star are annotated with subscript “c”. Quantities with subscript “core” correspond to mass averaged quantities over the iron core, e.g. . MCh is the Chandrasekhar mass as defined in Eq. (19). The explodability parameters ξM, M4 and μ4 are defined in Eqs. (24), (25) and (26), respectively. M4, g is the gravitational mass of a hypothetical neutron star resulting from the collapse of the core (Eq. (29)).
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