Table 2.
Fit results for the broadband light curve.
| Refreshed shocks | Off-axis jet | Cocoon I | Cocoon II | |
|---|---|---|---|---|
| log(Etot [erg]) | 48.43a | 51.17![]() |
51.52![]() |
50.93![]() |
| log(E0 [erg]) | 49.42![]() |
54.50![]() |
||
| log(γ0) | 1.59![]() |
|||
| log(ϵe) | −0.58![]() |
−0.60![]() |
−1.35![]() |
−0.51![]() |
| log(ϵB) | −1.30![]() |
−1.36![]() |
−0.89![]() |
−0.53![]() |
| log(A∗ [cm−1]) | −1.69![]() |
−0.49![]() |
||
| s | 2.46![]() |
|||
| p | 2.0 | 2.016![]() |
2.02![]() |
2.27![]() |
| θv | 0.108![]() |
|||
| u | 1.06![]() |
0.34![]() |
||
| log(n0 [cm−3]) | 3.45![]() |
3.90![]() |
||
Notes. In the first column, we list the parameters for each model: refreshed shock in the jet wings (second column), off-axis top-hat jet core (third column), and two cocoons describing the radio emission at ν < 20 GHz (fourth column) and at ν > 20 GHz (fifth column), respectively. In the second row, Etot indicates the beaming-corrected energy for the wings refreshed shock and off-axis jet core models, and the total kinetic energy for the two cocoon models.
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