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Fig. 4.

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Final binary evolution calculations for δov = 0.00, shown in the initial orbital period-secondary mass (log Pi, M2i) plane, where Pi represents the initial orbital period and M2i is the initial mass of the donor star (for various initial WD masses, as indicated in each panel). Filled squares indicate SN Ia explosions during the CE phase (the red indicates MCE > 0.1 M, the blue 0.1 M > MCE > 0). Filled circles denote SN Ia explosions in the SSS phase ( M ˙ cr | M ˙ 2 | 1 2 M ˙ cr $ \dot{M}_{\mathrm{cr}} \geq |\dot{M}_2| \geq \frac{1}{2} \dot{M}_{\mathrm{cr}} $ and MCE = 0), and filled triangles in the RN phase ( 1 2 M ˙ cr > | M ˙ 2 | 1 8 M ˙ cr $ \frac{1}{2} \dot{M}_{\mathrm{cr}} > |\dot{M}_2| \geq \frac{1}{8} \dot{M}_{\mathrm{cr}} $ and MCE = 0). Open circles represent systems that experience nova explosions, preventing the CO WD from reaching 1.378 M ( | M ˙ 2 | < 1 8 M ˙ cr $ |\dot{M}_2| < \frac{1}{8} \dot{M}_{\mathrm{cr}} $ and MCE = 0), while crosses show systems that are unstable due to dynamical mass transfer.

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