Fig. 13.
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Comparison of the bolometric light curves for model logP2p80 (solid; smooth ejecta) and model logP2p80fcl (dashed; clumped ejecta). For the clumped model, we adopt the same ejecta as for model logP2p80 but introduce a volume filling factor for the material, with a value of 10% up to about 12 000 km s−1 and rising steeply to asymptote at 100% beyond.
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