Table 6
γm,
, ϵB, Eiso, n and θ0 for the models described in Sects. 4.1–4.3. 
and Eiso,52 = Eiso/ 1052.
| γm |
|
ϵ B | A∗ , n0 | θ0 [rad] | Eiso,52[erg] | η | |
|
|
|||||||
| Jet break, p = 1.73 ± 0.03, νc<νKs | |||||||
|
|
|||||||
| ν sa < ν m |
|
|
|
|
|
|
|
| ν m < ν sa | < 11.2 | < 9.31 × 10-4 | < 7.87 × 10-2 | > 0.78 | > 0.13 | > 2.94 | < 74% |
|
|
|||||||
| Energy injection until tb in the light curve, p = 2.73 ± 0.03, νc>νxrt | |||||||
|
|
|||||||
| k = 2 | > 2.01 × 103 | > 1.10 | < 6.64 × 10-10 | > 1.23 × 103 | > 0.85 | > 2.36 | < 78% |
| k = 1.05 | > 1.4 × 103 | > 0.76 | < 2.1 × 10-9 | > 4.3 × 105 | > 0.8 | > 3.4 | < 71% |
| k = 0 | > 1.11 × 103 | > 0.75 | < 2.25 × 10-9 | > 1.21 × 107 | > 0.77 | > 3.67 | < 69% |
|
|
|||||||
| Energy injection scenario with jet break, p = 2.73 ± 0.03, νc>νxrt | |||||||
|
|
|||||||
| k = 0 | > 1.6 × 104 | > 7.6 | < 3.9 × 10-8 | > 1.29 × 107 | > 1.21 × 10-2 | > 0.16 | < 98% |
Notes. The half-opening angle is derived using Eq. (4) from Granot et al. (2005). n = Ar-2 with A = Ṁ/ 4πvw = 5 × 1011A∗ g cm-1 (Chevalier & Li 2000). For k = 2 we report the density in terms of A∗. For k = 0 and k = 1.05 we report the number density n0 in units of cm-3. In the special case of k = 1.05 we use a reference distance of r = 1017 cm.
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