Fig. 5.

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Example calculation for an interaction at a very late time in the nebular phase (black). The ejecta is limited to a 1 M⊙ dense shell moving at 10 000 km s−1 and powered at a rate of 3 × 1041 erg s−1. A uniform and strong clumping corresponding to a volume filling factor of 1% was used to compensate for the spatial spread of the dense shell (set to ∼10% of the local radius). This spectrum is reminiscent of the observations of SN 1993J at a similar epoch (red; Matheson et al. 2000). The observed spectrum was corrected for redshift and reddening, and then normalized at 4800 Å to match the model spectrum.
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