Fig. 9.

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SN2008D requires a strongly inverted 56Ni profile, with the external abundance of Xout = 0.71 in a layer that reaches the surface; in this case, the progenitor model is He5 with Eexp = 1 foe. The late LC decline is reproduced when passing from a fixed κγ = 0.03 cm2 g−1 opacity (dashed line) to half this value at t > 40 d (solid line). Lower panel: evolution of the photospheric velocity, although we did not use observational velocities to constrain the model. The velocities of the photosphere are taken from Tanaka et al. (2009b).
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