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Table 3.

Initial and final masses, mass lost through winds and size of the cores of the models computed in the present work.

Model Mini(M⊙) Mfin(M⊙) Mej,wind(M⊙) MHe(M⊙) MCO(M⊙) Mrem(M⊙)
10s0 10 9.93 0.07 2.91 1.58 1.28
10s4 10 9.78 0.22 3.35 1.86 1.36
15s0 15 14.78 0.22 4.67 2.62 1.56
15s4 15 14.34 0.66 5.74 3.36 1.75
20s0 20 19.87 0.13 6.46 4.04 1.92
20s4 20 17.36 2.64 8.21 5.31 2.24
25s0 25 24.68 0.32 8.65 5.88 2.39
25s4 25 16.68 8.32 10.85 7.53 2.80
25s7 25 16.21 8.79 10.91 7.56 2.81
25s7Ba 25 16.01 8.99 10.96 7.62 2.82
40s0 40 34.10 5.90 15.29 11.75 3.80
40s4 40 24.60 15.40 19.10 14.66 4.54
60s0 60 44.17 15.83 25.36 20.94 6.44
60s4 60 40.81 19.19 30.77 25.35 7.77
85s0 85 59.33 25.67 37.86 32.86 9.90
85s4 85 58.27 26.73 45.57 39.30 11.73
120s0 120 82.45 37.55 54.30 50.01 14.69
120s0Ba 120 83.18 36.82 54.46 49.35 14.51
120s4 120 85.81 34.19 65.28 61.78 17.95
150s0 150 100.26 49.74 70.77 65.34 18.94
150s4 150 99.59 50.41 83.83 80.04 23.04

Notes. Model label (Col. 1), initial mass (Col. 2), final mass (Col. 3), mass ejected through winds (Col. 4), mass of the H-free region (mass coordinate where the mass fraction of hydrogen X(1H) drops below 0.01, Col. 5), mass of the CO core (mass coordinate where the 4He mass fraction X(4He) drops below 0.01, Col. 6), remnant mass Mrem using the relation of Maeder (1992, Col. 7).

(a)

Models computed with the rate of 17O(α, γ) divided by 10.

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