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Table A.1

Most important parameters of simulated systems with f = 1.0 (see Sect. 2.2) at the point of He-ignition.

# Linit / 108 Minit t MHe,f T4,f Lf ρ6,c T8,ign ρ6,ign Mr,ign
[log (L/L)] [M/ yr] [M] [Myr] [M] [log (L/L)] [M]

Lm20510-1 2 1 0.54 69.55 0.70 13.27 1.45 39.49 1.94 11.98 0.50
Lm20510-2 2 2 0.54 30.72 0.61 8.33 0.71 25.84 2.08 6.32 0.56
Lm20510-3 2 3 0.54 7.64 0.229 4.99 0.37 4.36 3.42 0.19 0.62
Lm20510-4 2 4 0.54 4.54 0.182 4.62 0.35 3.67 3.33 0.13 0.59
Lm20510-5 2 5 0.54 3.11 0.155 4.08 0.23 3.35 3.41 0.09 0.58
Lm20510-6 2 6 0.54 2.30 0.138 4.53 0.41 3.23 3.17 0.08 0.57
Lm20510-7 2 7 0.54 1.79 0.125 4.91 0.54 3.14 3.02 0.08 0.57
Lm20510-8 2 8 0.54 1.45 0.116 5.24 0.66 3.07 2.92 0.07 0.57
Lm20510-9 2 9 0.54 1.20 0.108 5.47 0.74 3.02 2.85 0.07 0.56
Lm20510-10 2 10 0.54 1.02 0.102 5.64 0.80 2.97 2.82 0.07 0.56

Lm10510-1 1 1 0.54 69.40 0.69 16.50 1.83 44.29 0.82 1.23 0.51
Lm10510-2 1 2 0.54 31.03 0.62 7.81 0.59 26.83 1.87 6.63 0.56
Lm10510-3 1 3 0.54 6.52 0.196 4.31 0.22 3.65 3.62 0.15 0.58
Lm10510-4 1 4 0.54 3.84 0.154 4.03 0.20 3.14 3.42 0.10 0.56
Lm10510-5 1 5 0.54 2.68 0.134 3.99 0.22 2.97 3.30 0.08 0.56
Lm10510-6 1 6 0.54 1.99 0.119 4.46 0.41 2.89 3.08 0.08 0.55
Lm10510-7 1 7 0.54 1.57 0.110 4.83 0.55 2.84 2.97 0.07 0.55
Lm10510-8 1 8 0.54 1.30 0.104 5.07 0.64 2.80 2.91 0.07 0.55
Lm10510-9 1 9 0.54 1.07 0.097 5.36 0.74 2.76 2.84 0.07 0.55
Lm10510-10 1 10 0.54 0.92 0.092 5.50 0.79 2.73 2.81 0.06 0.55

L00510-1 0 1 0.54 69.50 0.69 12.69 1.37 39.27 1.88 11.98 0.49
L00510-2 0 2 0.54 30.58 0.61 8.85 0.82 25.55 1.74 6.31 0.56
L00510-3 0 3 0.54 5.58 0.167 4.78 0.36 3.34 3.01 0.17 0.56
L00510-4 0 4 0.54 3.18 0.127 3.66 0.08 2.82 3.22 0.08 0.55
L00510-5 0 5 0.54 2.17 0.109 4.24 0.33 2.69 2.95 0.07 0.55
L00510-6 0 6 0.54 1.62 0.097 4.60 0.47 2.61 2.80 0.07 0.54
L00510-7 0 7 0.54 1.25 0.088 4.91 0.59 2.55 2.68 0.06 0.54
L00510-8 0 8 0.54 1.01 0.081 4.83 0.59 2.50 2.70 0.05 0.54
L00510-9 0 9 0.54 0.87 0.078 4.98 0.67 2.49 2.72 0.05 0.54
L00510-10 0 10 0.54 0.71 0.071 5.39 0.78 2.46 2.60 0.05 0.54

Lm20810-1 2 1 0.82 48.46 0.48 7.98 0.43 66.99 2.01 10.61 0.78
Lm20810-2 2 2 0.82 21.17 0.42 8.36 0.59 46.57 2.15 5.77 0.83
Lm20810-3 2 3 0.82 8.27 0.248 8.29 0.77 19.28 1.75 0.60 0.97
Lm20810-4 2 4 0.82 4.60 0.184 6.95 0.64 14.30 4.11 0.22 0.92
Lm20810-5 2 5 0.82 3.09 0.154 6.92 0.68 12.90 3.86 0.16 0.90
Lm20810-6 2 6 0.82 2.26 0.136 6.71 0.68 12.11 3.97 0.12 0.89
Lm20810-7 2 7 0.82 1.51 0.105 7.75 0.88 11.72 3.38 0.13 0.87
Lm20810-8 2 8 0.82 0.71 0.057 8.74 0.98 12.98 3.45 0.12 0.84
Lm20810-9 2 9 0.82 0.49 0.044 8.78 0.99 13.03 3.76 0.10 0.84
Lm20810-10 2 10 0.82 0.37 0.037 9.40 1.08 13.03 3.61 0.10 0.83

Lm10810-1 1 1 0.82 48.49 0.48 7.61 0.35 67.15 2.01 10.47 0.78
Lm10810-2 1 2 0.82 21.12 0.42 8.33 0.59 46.33 2.14 5.75 0.83
Lm10810-3 1 3 0.82 7.51 0.225 8.20 0.78 17.25 1.71 0.58 0.94
Lm10810-4 1 4 0.82 4.17 0.167 6.94 0.65 13.10 3.91 0.23 0.90
Lm10810-5 1 5 0.82 2.83 0.142 6.79 0.67 11.97 3.92 0.17 0.89
Lm10810-6 1 6 0.82 1.59 0.095 6.44 0.62 11.44 4.24 0.12 0.86
Lm10810-7 1 7 0.82 0.74 0.051 7.53 0.77 12.51 4.32 0.11 0.83
Lm10810-8 1 8 0.82 0.51 0.041 9.20 1.03 12.72 3.69 0.13 0.83
Lm10810-9 1 9 0.82 0.38 0.034 8.87 1.00 12.61 3.84 0.10 0.83
Lm10810-10 1 10 0.82 0.30 0.030 9.40 1.09 12.58 3.67 0.10 0.82

L00810-1 0 1 0.82 48.57 0.49 8.43 0.53 67.09 2.01 10.61 0.78
L00810-2 0 2 0.82 21.21 0.42 8.36 0.59 46.48 2.13 5.83 0.83
L00810-3 0 3 0.82 7.21 0.216 8.15 0.78 16.52 1.70 0.57 0.93
L00810-4 0 4 0.82 3.93 0.157 6.76 0.62 12.46 4.06 0.22 0.89
L00810-5 0 5 0.82 0.94 0.047 7.46 0.70 12.27 4.23 0.15 0.82
L00810-6 0 6 0.82 0.56 0.034 7.48 0.72 12.16 4.27 0.11 0.82
L00810-7 0 7 0.82 0.34 0.024 8.79 0.97 12.17 3.77 0.10 0.82
L00810-8 0 8 0.82 0.30 0.024 8.83 0.98 12.10 3.75 0.10 0.82
L00810-9 0 9 0.82 0.24 0.022 9.38 1.08 12.06 3.59 0.10 0.82
L00810-10 0 10 0.82 0.20 0.020 7.63 0.85 11.84 4.45 0.06 0.82

Lm21010-4 2 4 1.00 2.01 0.080 10.29 0.95 40.94 4.68 0.27 1.05
Lm21010-5 2 5 1.00 0.64 0.032 9.52 0.83 38.03 4.96 0.14 1.01
Lm21010-6 2 6 1.00 0.33 0.020 11.12 1.10 36.58 4.43 0.12 1.00
Lm21010-7 2 7 1.00 0.21 0.015 11.41 1.14 35.86 4.13 0.11 1.00
Lm21010-8 2 8 1.00 0.15 0.012 11.65 1.17 35.50 3.89 0.11 1.00
Lm21010-9 2 9 1.00 0.12 0.010 10.92 1.10 35.14 4.48 0.08 1.00
Lm21010-10 2 10 1.00 0.09 0.009 11.13 1.14 34.97 4.46 0.07 1.00

Lm11010-4 1 4 1.00 0.89 0.035 9.42 0.80 37.40 5.17 0.21 1.01
Lm11010-5 1 5 1.00 0.41 0.020 10.91 1.07 35.68 4.74 0.14 1.00
Lm11010-6 1 6 1.00 0.24 0.015 10.48 1.00 34.93 4.41 0.12 1.00
Lm11010-7 1 7 1.00 0.17 0.012 11.15 1.10 34.58 4.00 0.11 1.00
Lm11010-8 1 8 1.00 0.12 0.010 10.60 1.06 34.24 4.49 0.08 1.00
Lm11010-9 1 9 1.00 0.10 0.009 10.76 1.09 34.06 4.51 0.07 1.00
Lm11010-10 1 10 1.00 0.08 0.008 11.27 1.18 33.94 4.50 0.06 1.00

L01010-4 0 4 1.00 0.35 0.014 9.56 0.86 33.79 4.53 0.12 1.00
L01010-5 0 5 1.00 0.21 0.010 10.31 0.97 33.32 3.91 0.11 1.00
L01010-6 0 6 1.00 0.15 0.009 9.85 0.95 32.95 4.47 0.07 1.00
L01010-7 0 7 1.00 0.11 0.008 10.85 1.13 32.77 4.48 0.06 1.00
L01010-8 0 8 1.00 0.09 0.007 11.94 1.31 32.63 4.52 0.05 1.00
L01010-9 0 9 1.00 0.07 0.006 12.84 1.44 32.54 4.50 0.05 1.00
L01010-10 0 10 1.00 0.06 0.006 13.43 1.52 32.51 4.47 0.05 1.00

Lm11110-4 1 4 1.10 0.35 0.014 11.20 0.95 73.91 5.45 0.15 1.11
Lm11110-5 1 5 1.10 0.20 0.010 11.72 1.01 72.65 4.60 0.14 1.10
Lm11110-6 1 6 1.10 0.13 0.008 16.78 1.76 71.27 5.99 0.07 1.10
Lm11110-7 1 7 1.10 0.10 0.007 19.61 2.05 70.91 6.00 0.06 1.10
Lm11110-8 1 8 1.10 0.07 0.006 24.90 2.51 70.41 6.00 0.05 1.10
Lm11110-9 1 9 1.10 0.06 0.005 28.76 2.79 70.18 6.00 0.04 1.10
Lm11110-10 1 10 1.10 0.05 0.005 32.16 3.01 70.00 6.00 0.04 1.10

L01110-4 0 4 1.10 0.20 0.008 10.67 0.87 68.70 4.64 0.12 1.10
L01110-5 0 5 1.10 0.13 0.006 19.38 2.05 67.72 6.00 0.06 1.10
L01110-6 0 6 1.10 0.09 0.006 23.09 2.38 67.38 6.00 0.05 1.10
L01110-7 0 7 1.10 0.07 0.005 27.35 2.71 67.12 6.00 0.04 1.10
L01110-8 0 8 1.10 0.06 0.004 32.29 3.04 66.90 6.00 0.03 1.10
L01110-9 0 9 1.10 0.05 0.004 36.19 3.28 66.73 6.00 0.03 1.10
L01110-10 0 10 1.10 0.04 0.004 39.39 3.47 66.59 6.00 0.02 1.10

Notes. The leftmost column lists the model number. Linit is the luminosity at the start of mass accretion, the accretion rate, Minit the initial mass of the model, t the time since the start of mass accretion, MHe,f the mass of the accumulated He-envelope at the time of ignition, T4,f the effective temperature at the time of ignition in units of 104 K, Lf the luminosity at ignition, ρ6,c the core density at the time of ignition in units of [106 g/cm3], T8,ign the temperature the point of ignition in units of [108 K], ρ6,ign the density at the point of ignition in units of [106 g/cm3] and Mr,ign the location of the point of ignition expressed in terms of the mass coordinate. The model number is composed as follows: the first digit indicates the value of the initial luminosity, if preceded by the letter “m”, that value should be understood to be negative. The second and third digits are equal to ten times value of the initial mass rounded to the next 0.1 M. The fourth and fifth digits are equal to the value of ten times the chosen value for f. The hyphenated number is equal to the value of the chosen mass accretion rate divided by 10-8.

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