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Table A.1.

Selected properties of the evolution models.

Mini αov D tH Mc,He M∗,H tHe Mc,C M∗,He (C/O)c 22Netot M , C $ _{*,\rm C} $ ttot ΔM log( T c , f K $ \frac{T_{c,f}}{K} $) log( ρ c , f g c m 3 ) $ \frac{\rho_{c,f}}{g*cm^{-3}}) $
(M) - - (Myr) (M) (M) (Myr) (M) (M) - (M) (M) (Myr) (M) - -
20 0.05 0 8.09 4.62 19.9 0.797 4.55 14.8 0.441 0.0256 14.6 9.01 5.39 8.97 5.98
20 0.05 1.5 8.11 4.63 19.9 0.793 4.47 15.2 0.455 0.0263 15 9.03 4.96 8.97 6
20 0.05 3 8.11 4.64 19.9 0.81 4.52 14.8 0.425 0.0257 14.6 9.04 5.4 8.98 5.96
20 0.05 4.5 8.08 4.61 19.9 0.813 4.29 15.2 0.413 0.0249 15.1 9.02 4.94 8.98 5.97
20 0.05 6 8.74 5.03 19.8 1.15 3.22 10.9 0.247 0.146 10.7 10.0 9.27 8.84 5.53

20 0.1 0 8.25 4.97 19.9 0.741 4.58 15.9 0.479 0.0275 15.8 9.11 4.25 8.97 6.02
20 0.1 1.5 8.25 4.97 19.9 0.737 4.69 15.4 0.469 0.0273 15.3 9.11 4.75 8.97 5.99
20 0.1 3 8.25 4.98 19.9 0.739 4.66 15.5 0.467 0.0179 15.4 9.11 4.61 8.97 5.98
20 0.1 4.5 8.29 4.99 19.9 0.748 4.60 15.1 0.431 0.0262 14.9 9.15 5.06 8.98 5.95
20 0.1 6 8.99 5.41 19.7 0.997 3.93 10.6 0.23 0.0771 10.4 10.1 9.62 8.99 6.08

20 0.2 0 8.72 5.71 19.7 0.672 5.6 12.9 0.43 0.0256 12.7 9.48 7.29 9 5.32
20 0.2 1.5 8.72 5.71 19.7 0.673 5.59 12.9 0.431 0.0258 12.8 9.48 7.24 9 5.32
20 0.2 3 8.72 5.71 19.7 0.672 5.57 13.0 0.43 0.0257 12.9 9.48 7.13 9 5.32
20 0.2 4.5 8.75 5.74 19.7 0.681 5.41 13.2 0.409 0.025 13.0 9.53 6.95 9 5.33
20 0.2 6 9.42 6.21 19.6 0.811 4.97 10.1 0.224 0.0362 9.99 10.3 10 9 5.85

20 0.4 0 9.50 7.16 19.5 0.582 6.88 11.4 0.403 0.0235 11.2 10.2 8.75 9 5.22
20 0.4 1.5 9.50 7.16 19.5 0.583 6.87 11.4 0.404 0.0237 11.3 10.2 8.74 9 5.23
20 0.4 3 9.50 7.16 19.5 0.583 6.87 11.4 0.403 0.0236 11.3 10.2 8.74 9 5.24
20 0.4 4.5 9.54 7.2 19.5 0.587 6.76 11.3 0.384 0.0226 11.2 10.2 8.79 9 5.67
20 0.4 6 10.1 7.79 19.3 0.66 6.64 9.83 0.232 0.0198 9.73 10.9 10.3 9 5.63

Notes. We note that Mini is the initial mass in M; αov the amount of CBM on the main sequence; D is short for log(Denv/cm2s−1), the amount of envelope mixing; tH, tHe, and ttot the duration of hydrogen burning, helium burning, and the total evolution time in millions of years, respectively. We note that M∗,H, M∗,He, and M∗,C are the masses of the stars at the end of their respective burning phases in M; Mc,He and Mc,C the masses of the hydrogen- and the helium-depleted core, respectively, at the end of the corresponding burning phases in M; (C/O)c is the carbon-over-oxygen ratio of the core at the end of helium burning; 22Netot gives the total mass of 22Ne at the end of helium burning in M, ΔM the total mass lost in M; Tc, f is the final core temperature in K and ρc, f is the final core density in g/cm3.

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