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Table 2.

Key parameters for the binary models reran in this work.

Case B RLOF Core He burning Core He-dep Case BC RLOF End
M1, i Pi ΔM1 ΔM2 Δt M conv max$ M_{\mathrm {conv}}^{\mathrm {max}} $ L ℒ Teff M1 RRL, 1 Δt ΔM1 M ˙ max ( − 4 )$ \dot M_{\mathrm {max}}^{(-4)} $ Δtmax M1 (†) MCO (†) 〈Z〉env (†) log ρc log Tc log Tmax End
( M⊙) (d) ( M⊙) ( M⊙) (Myr) ( M⊙) (k L⊙) (kℒ⊙) (kK) ( M⊙) ( R⊙) ( kyr) ( M⊙) ( kyr) ( M⊙) ( M⊙) (g cm−3) (K) (K) of run
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10) (11) (12) (13) (14) (15) (16) (17) (18) (19) (20) (21) (22)
12.3 5.01 8.61 0.26 1.72 1.30 8.66 3.02 80.0 2.53 5.88 26.1 0.79 1.18 4.19 1.62 1.44 0.14 7.68 8.68 9.27 NeEC
12.3 6.31 8.57 0.21 1.67 1.32 9.30 3.16 80.1 2.58 7.51 23.2 0.78 1.35 3.61 1.68 1.46 0.19 8.71 9.00 9.42 Ne/O/Si (*)
12.3 10.0 8.50 0.18 1.60 1.36 10.5 3.43 79.9 2.66 11.8 13.7 0.74 1.95 2.64 1.81 1.50 0.19 8.26 9.07 9.51 Ne/O/Si
12.3 15.8 8.45 0.15 1.53 1.38 11.5 3.64 79.3 2.73 18.1 8.44 0.70 2.85 1.95 1.92 1.53 0.16 8.26 9.11 9.43 Ne/O
12.3 25.1 8.42 0.15 1.49 1.40 12.2 3.79 78.7 2.78 27.1 4.98 0.57 3.10 1.15 2.10 1.55 0.12 8.21 9.12 9.39 O
12.3 39.8 8.39 0.16 1.45 1.41 12.8 3.91 78.1 2.83 40.1 2.22 0.41 2.92 0.67 2.30 1.57 0.10 8.83 9.21 9.58 Si (*)
12.3 63.1 8.36 0.16 1.43 1.42 13.2 4.01 77.6 2.86 58.2 1.52 0.28 2.85 0.02 2.46 1.58 0.09 8.79 9.34 9.55 Si
12.3 100 8.35 0.16 1.43 1.44 13.6 4.08 77.2 2.88 83.5 1.13 0.18 2.96 0.02 2.58 1.59 0.08 8.84 9.34 9.55 Si
12.3 158 8.33 0.17 1.43 1.46 13.8 4.13 77.1 2.89 119 0.78 0.10 1.75 0.15 2.67 1.61 0.07 8.68 9.35 9.55 Si
12.3 251 8.32 0.16 1.43 1.47 14.0 4.18 76.8 2.90 168 / / / / 2.78 1.62 0.06 7.80 9.07 9.50 Ne/O/Si
12.6 5.01 8.75 0.26 1.64 1.37 9.59 3.22 81.2 2.62 5.92 22.5 0.78 1.28 3.27 1.72 1.48 0.20 8.55 9.03 9.44 Ne/O/Si (*)
12.6 6.31 8.71 0.20 1.59 1.40 10.3 3.38 81.4 2.67 7.56 19.5 0.76 1.49 2.73 1.79 1.51 0.20 7.93 9.01 10.2 Ne/O/Si
12.6 10.0 8.64 0.19 1.52 1.44 11.6 3.65 81.2 2.75 11.8 10.4 0.71 2.30 1.84 1.93 1.56 0.18 8.85 9.21 9.57 Si (*)
12.6 15.9 8.59 0.15 1.47 1.46 12.6 3.86 80.6 2.82 18.1 5.70 0.54 2.79 0.94 2.16 1.59 0.13 8.85 9.33 9.56 Si (*)
12.6 25.1 8.55 0.13 1.42 1.48 13.4 4.02 80.0 2.87 27.1 2.24 0.31 2.57 0.37 2.45 1.61 0.09 8.70 9.23 9.57 Si (*)
12.6 39.8 8.52 0.16 1.39 1.49 14.0 4.15 79.4 2.92 40.1 1.16 0.16 2.26 0.04 2.64 1.63 0.08 8.63 9.34 9.56 Si (*)
12.6 63.1 8.49 0.17 1.37 1.50 14.5 4.25 79.0 2.95 58.1 0.65 0.06 1.65 0.04 2.77 1.64 0.07 8.78 9.37 9.55 Si (*)
12.6 100 8.48 0.17 1.36 1.51 14.9 4.32 78.6 2.97 83.3 0.28 0.01 1.34 0.02 2.84 1.65 0.07 8.70 9.24 9.57 Si (*)
12.9 5.01 8.89 0.32 1.56 1.45 10.6 3.43 82.5 2.70 5.90 19.26 0.77 1.38 2.50 1.81 1.53 0.21 9.09 9.31 9.51 Si (*)
12.9 6.31 8.84 0.21 1.52 1.49 11.4 3.60 82.6 2.76 7.59 15.35 0.74 1.70 1.99 1.90 1.56 0.20 8.57 9.26 9.38 Si
12.9 10.0 8.77 0.20 1.46 1.52 12.7 3.87 82.5 2.83 11.8 7.66 0.61 2.49 1.06 2.11 1.62 0.14 8.76 9.21 9.57 Si (*)
12.9 15.9 8.72 0.16 1.41 1.55 13.8 4.09 82.1 2.90 18.1 3.47 0.29 2.53 0.02 2.50 1.65 0.10 8.85 9.45 9.98 Si (*)
12.9 25.1 8.68 0.16 1.37 1.56 14.7 4.26 81.5 2.96 27.0 1.04 0.10 1.87 0.03 2.75 1.68 0.08 9.02 9.40 10.0 Si (*)
12.9 39.8 8.65 0.16 1.34 1.58 15.3 4.38 81.0 3.00 40.1 0.40 0.02 1.04 0.03 2.86 1.69 0.08 8.56 9.43 9.57 Si (*)
12.9 63.1 8.62 0.17 1.32 1.59 15.9 4.49 80.5 3.03 58.0 / / / / 2.92 1.71 0.07 8.46 9.44 9.56 Si
13.2 5.01 9.02 0.29 1.49 1.53 11.7 3.67 83.7 2.79 6.01 16.1 0.76 1.54 1.77 1.92 1.59 0.21 8.90 9.33 9.54 Si (*)
13.2 6.31 8.98 0.26 1.45 1.56 12.5 3.83 83.8 2.84 7.59 11.4 0.71 1.96 1.29 2.02 1.62 0.18 8.84 9.35 9.55 Si (*)
13.2 10.0 8.90 0.20 1.39 1.61 14.0 4.11 83.8 2.93 11.9 5.30 0.41 2.40 0.33 2.41 1.68 0.10 8.41 9.42 9.57 Si
13.2 15.9 8.84 0.16 1.35 1.64 15.1 4.33 83.4 2.99 18.1 1.35 0.10 1.79 0.02 2.77 1.72 0.08 8.30 9.53 9.57 Si
13.2 25.1 8.80 0.14 1.32 1.66 16.1 4.52 82.9 3.05 27.2 0.26 0.01 0.57 0.03 2.93 1.75 0.08 8.71 9.52 9.55 Si (*)
13.2 39.8 8.77 0.16 1.29 1.67 16.8 4.65 82.4 3.09 40.1 / / / / 2.98 1.76 0.08 8.27 9.53 9.56 Si
13.5 5.01 9.15 0.29 1.42 1.63 13.0 3.91 84.9 2.89 6.07 13.0 0.72 1.75 1.12 2.05 1.66 0.17 8.77 9.38 9.55 Si (*)
13.5 6.31 9.11 0.27 1.38 1.66 13.8 4.08 85.1 2.94 7.62 8.57 0.60 2.15 0.60 2.23 1.69 0.13 9.00 9.37 9.43 Si (*)
13.5 10.0 9.03 0.21 1.33 1.71 15.3 4.36 85.1 3.02 11.9 3.41 0.18 2.08 0.02 2.72 1.74 0.09 8.73 9.24 9.57 Si (*)
13.5 15.9 8.97 0.16 1.29 1.73 16.5 4.58 84.8 3.08 18.2 0.50 0.02 0.76 0.01 2.95 1.78 0.09 8.74 9.50 9.55 Si (*)
13.5 25.1 8.92 0.14 1.26 1.75 17.6 4.77 84.3 3.14 27.2 / / / / 3.03 1.81 0.08 7.86 9.54 9.57 Si
13.8 5.01 9.28 0.31 1.36 1.72 14.3 4.15 86.1 2.98 6.12 10.2 0.63 1.94 0.55 2.24 1.72 0.15 8.44 9.35 9.56 Si (*)
13.8 6.31 9.24 0.28 1.32 1.75 15.2 4.33 86.3 3.03 7.61 6.38 0.40 2.36 0.02 2.52 1.76 0.12 8.22 9.53 9.56 Si
13.8 10.0 9.16 0.21 1.28 1.80 16.7 4.61 86.4 3.11 12.0 1.66 0.05 1.14 0.01 2.95 1.81 0.09 7.86 9.51 9.54 Si
13.8 15.9 9.10 0.17 1.24 1.84 18.1 4.84 86.1 3.18 18.3 / / / / 3.07 1.84 0.09 10.1 10.0 10.0 CC
14.1 5.01 9.41 0.32 1.30 1.83 15.7 4.41 87.3 3.08 6.18 7.56 0.44 2.14 0.02 2.53 1.79 0.12 7.88 9.54 9.57 Si
14.1 6.31 9.37 0.31 1.26 1.86 16.7 4.59 87.6 3.13 7.66 4.51 0.21 1.76 0.01 2.81 1.82 0.10 7.83 9.52 9.55 Si
14.1 10.0 9.28 0.23 1.22 1.91 18.3 4.87 87.7 3.21 12.0 0.43 0.01 0.41 0.01 3.09 1.88 0.09 10.2 10.0 10.0 CC
14.1 15.9 9.22 0.17 1.19 1.94 19.7 5.11 87.4 3.28 18.3 / / / / 3.17 1.92 0.09 10.2 10.0 10.0 CC

Notes. The rows are grouped by models with the same initial primary mass M1. The columns are divided in different groups, for different evolutionary phases. Columns 1 and 2 show the initial conditions: the initial primary mass (Col. 1) and initial orbital period (2). Columns 3 and 4 show the amount of mass shed by the primary (3) and accreted by the secondary (4) during Case B RLOF. Columns 5–9 show parameters during core He burning: the time spent in this phase (5), the maximum extent in mass of the convective core (6), the average luminosity, spectroscopic luminosity and effective temperature of the primary (7–9, with a standard deviation of about ∼10%). Columns 10–11 show the parameters at core He depletion: the mass of the primary (10) and the Roche lobe radius (11). Columns 12–15 show parameters associated to Case BC RLOF: the time between the end of the run and the onset of Case BC RLOF (12), the amount of mass shed by the primary (13), the maximum mass transfer rate in units of 10−4 M⊙ yr−1 (14) and the time before the end of the run at which the maximum mass transfer rate was reached (15). Columns 16–22 show the parameters at the end of the run: the final mass of the primary (16), its CO-core mass (17), the average metal abundance in the envelope (18), central density and temperature (19–20), the maximum temperature (21) and the burning phase at the end of the run labeled according to the nuclei being burnt, if it didn’t reach CC (22). (*)Models have experienced Case X RLOF (see Sect. 4.2.3). (EC) The least-massive model is expected to end as an EC-SN. (†)The data is taken at 1 year before the end of the run to filter out the effects of Case X RLOF.

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