Fig. 2
Calculation results for Case II: L0 = 1049 erg s-1, Mej = 10-4M⊙. Descriptions of panels are the same as in Fig. 1. In panel a) the blast wave decelerates immediately after linearly accelerating. In panels c) and d), owing to more energy injection to the blast wave than Case I, both reverse shock and forward shock emission is stronger than in Case I.
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