Table 3
Model summary at the end of the mass loss phase (when Tc ≥ 109 K, roughly corresponding to neon core ignition).
End of mass loss phase: Tc ≥ 109 K | |||||||||
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MZAMS = 15 M⊙ | MZAMS = 20 M⊙ | ||||||||
η | ID | M [ M⊙ ] | MHe [ M⊙ ] | MCO [ M⊙ ] | η | ID | M [ M⊙ ] | MHe [ M⊙ ] | MCO [ M⊙ ] |
|
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0.1 | V-dJ | 14.66 | 4.99 | 3.20 | 0.1 | V-dJ | 19.23 | 7.04 | 4.91 |
V-NJ | 14.64 | 4.99 | 3.20 | V-NJ | 19.23 | 7.04 | 4.91 | ||
V-vL | 13.60 | 4.98 | 3.20 | V-vL | 18.10 | 7.03 | 4.91 | ||
K-dJ | 14.67 | 5.00 | 3.22 | K-dJ | 19.38 | 7.01 | 4.90 | ||
K-NJ | 14.66 | 5.00 | 3.22 | K-NJ | 19.37 | 7.01 | 4.90 | ||
K-vL | 13.61 | 5.00 | 3.21 | K-vL | 18.67 | 7.01 | 4.90 | ||
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0.33 | V-dJ | 13.94 | 4.93 | 3.16 | 0.33 | V-dJ | 17.47 | 7.01 | 4.88 |
V-NJ | 13.90 | 4.93 | 3.16 | V-NJ | 17.48 | 7.01 | 4.88 | ||
V-vL | 10.39 | 4.93 | 3.15 | V-vL | 13.47 | 6.99 | 4.87 | ||
K-dJ | 13.92 | 4.98 | 3.19 | K-dJ | 17.62 | 7.00 | 4.87 | ||
K-NJ | 13.88 | 4.98 | 3.19 | K-NJ | 17.62 | 7.00 | 4.88 | ||
K-vL | 10.11 | 4.97 | 3.19 | K-vL | 13.90 | 6.98 | 4.87 | ||
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|
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1.0 | V-dJ | 12.86 | 4.65 | 2.95 | 1.0 | V-dJ | 11.81 | 7.06 | 4.92 |
V-NJ | 12.74 | 4.65 | 2.95 | V-NJ | 12.04 | 7.06 | 4.92 | ||
V-vL | 5.25 | 4.64 | 2.94 | V-vL | 8.80 | 7.02 | 4.89 | ||
K-dJ | 11.97 | 4.92 | 3.15 | K-dJ | 12.62 | 6.95 | 4.84 | ||
K-NJ | 11.87 | 4.92 | 3.14 | K-NJ | 12.77 | 6.95 | 4.84 | ||
K-vL | 5.70 | 4.90 | 3.13 | K-vL | 8.81 | 6.90 | 4.80 | ||
|
|||||||||
MZAMS = 25 M⊙ | MZAMS = 30 M⊙ | ||||||||
η | ID | M [ M⊙ ] | MHe [ M⊙ ] | MCO [ M⊙ ] | η | ID | M [ M⊙ ] | MHe [ M⊙ ] | MCO [ M⊙ ] |
|
|||||||||
0.1 | V-dJ | 23.85 | 9.14 | 6.58 | 0.1 | V-dJ | 28.11 | 10.97 | 7.97 |
V-NJ | 23.86 | 9.14 | 6.59 | V-NJ | 28.17 | 10.97 | 7.94 | ||
V-vL | 23.56 | 9.14 | 6.59 | V-vL | 28.70 | 10.96 | 7.95 | ||
K-dJ | 23.74 | 9.23 | 6.66 | K-dJ | 28.13 | 10.91 | 7.90 | ||
K-NJ | 23.76 | 9.24 | 6.67 | K-NJ | 28.19 | 10.91 | 7.86 | ||
K-vL | 23.24 | 9.23 | 6.67 | K-vL | 28.75 | 10.90 | 7.91 | ||
|
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|
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0.33 | V-dJ | 21.98 | 8.87 | 6.37 | 0.33 | V-dJ | 24.16 | 11.11 | 8.13 |
V-NJ | 22.02 | 8.87 | 6.38 | V-NJ | 24.34 | 11.11 | 8.13 | ||
V-vL | 22.13 | 8.87 | 6.36 | V-vL | 26.02 | 11.10 | 8.12 | ||
K-dJ | 21.27 | 9.11 | 6.57 | K-dJ | 25.03 | 10.89 | 7.88 | ||
K-NJ | 21.34 | 9.11 | 6.57 | K-NJ | 25.18 | 10.89 | 7.87 | ||
K-vL | 20.26 | 9.11 | 6.55 | K-vL | 27.12 | 10.87 | 7.80 | ||
|
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1.0 | V-dJ | 13.29 | 9.05 | 6.50 | 1.0 | V-dJ | 15.36 | 11.28 | 8.23 |
V-NJ | 13.67 | 9.05 | 6.48 | V-NJ | 15.78 | 11.29 | 8.26 | ||
V-vL | 12.97 | 9.04 | 6.51 | V-vL | 18.29 | 11.31 | 8.27 | ||
K-dJ | 15.57 | 8.89 | 6.38 | K-dJ | 18.51 | 10.92 | 7.96 | ||
K-NJ | 15.84 | 8.89 | 6.37 | K-NJ | 18.80 | 10.92 | 7.94 | ||
K-vL | 14.69 | 8.90 | 6.38 | K-vL | 22.53 | 10.89 | 7.94 | ||
|
|||||||||
MZAMS = 35 M⊙ | |||||||||
η | ID | M [ M⊙ ] | MHe [ M⊙ ] | MCO [ M⊙ ] | |||||
|
|||||||||
|
|||||||||
0.1 | V-dJ-NL | 32.61 | 10.25 | 7.19 | |||||
V-NJ-NL | 32.69 | 10.24 | 7.19 | ||||||
V-vL-NL | 33.99 | 10.03 | 7.03 | ||||||
K-dJ-NL | 32.43 | 11.87 | 8.54 | ||||||
K-NJ-NL | 32.53 | 11.87 | 8.56 | ||||||
K-vL-NL | 33.97 | 11.83 | 8.51 | ||||||
|
|||||||||
0.33 | V-dJ-NL | 27.36 | 12.72 | 9.32 | |||||
V-NJ-NL | 27.62 | 12.72 | 9.32 | ||||||
V-vL-NL | 31.40 | 12.67 | 9.23 | ||||||
K-dJ-NL | 27.50 | 12.68 | 9.21 | ||||||
K-NJ-NL | 27.78 | 12.68 | 9.28 | ||||||
K-vL-NL | 31.76 | 12.63 | 9.21 | ||||||
|
|||||||||
1.0 | V-dJ-NL | 20.03 | 13.30 | 9.81 | |||||
V-NJ-NL | 20.20 | 13.30 | 9.94 | ||||||
V-vL-NL | 24.85 | 13.30 | 9.97 | ||||||
K-dJ-NL | 20.32 | 13.82 | 10.33 | ||||||
K-NJ-NL | 20.45 | 13.82 | 10.36 | ||||||
K-vL-NL | 25.13 | 13.82 | 10.41 | ||||||
V-dJ-H | 19.73 | 13.30 | 9.93 | ||||||
V-NJ-H | 19.93 | 13.30 | 9.99 | ||||||
K-dJ-H | 19.48 | 13.81 | 10.41 | ||||||
K-NJ-H | 19.69 | 13.82 | 10.41 | ||||||
|
Notes. We provide total mass M, helium core mass MHe, and carbon-oxygen (CO) core mass MCO. We omit models differing only by the WR wind scheme if they do not reach the WR stage (i.e. Xs> 0.4 at all times). We define the edge of the CO core as first location going inward where X(4He) < 0.01, without requiring a minimum mass fraction of carbon or oxygen. Analogously, we define the outer edge of the helium core as the first location going inward where X(1H) < 0.01.
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