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Fig. 1.

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Light curve comparison between the SN observations (gray markers; Chen et al. 2024 bolometric) and the bolometric output from our double-peaked 56Ni distribution model. The inner component of the distribution is varied, while a fixed outer component of the profile is set to provide a reasonable fit for the first maximum of the LC. The model including a magnetar component is shown in magenta. In all the cases, the external enriched 56Ni shell is fixed, and the progenitor is the He11, as detailed in the text.

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