Table 1.
Parameters of numerical calculations.
| Model | Γ |
 |
 |
 |
R0 | s | g |
|---|---|---|---|---|---|---|---|
| (104) | (102 G) | (1047 s−1) | (cm) | ||||
| C1R14Γ240 | 240 | 2 | 2 | 4 | 1014 | ||
| C1R15Γ120 | 120 | 10 | 1 | 16 | 1015 | ||
| C2R14Γ240 | 240 | 2 | 2 | 64 | 1014 | ||
| C2R15Γ460 | 460 | 5 | 1 | 2 | 1015 | ||
| C3R14Γ1900 | 1900 | 1.4 | 3 | 1.2 | 1014 | ||
| C3R15Γ1900 | 1900 | 1.4 | 3 | 1.2 | 1015 | ||
| C4R14Γ460 | 460 | 5 | 0.8 | 4 | 1014 | ||
| AR14Γ200 | 200 | 3.5 | 0.6 | 20 | 1014 | 0.35 | |
| AR14Γ150 | 150 | 3.5 | 0.6 | 20 | 1014 | 0.55 | |
| A14Γ80 | 80 | 3.5 | 1.0 | 80 | 1014 | 1.0 | |
| AR15Γ230 | 230 | 5 | 2 | 8 | 1015 | 1.0 | |
| AG1R14Γ300 | 300 | 4.5 | 0.6 | 32 | 1014 | 0.0 | 0.7 |
| AG214Γ150 | 150 | 5.0 | 0.6 | 20 | 1014 | 0.55 | 0.5 |
| AG1R15Γ250 | 250 | 5 | 2 | 8 | 1015 | 0.0 | 1.0 |
| AG2R15Γ230 | 230 | 5 | 2 | 8 | 1015 | 1.0 | 1.0 |
Notes. Three distinct groups of cases are listed. In the fist group, letter C in the model name denotes that the shell is moving at a constant Lorentz factor, the numbers (1–4) signify that the cooling process is dominated by synchrotron cooling, SSC cooling, adiabatic cooling, or SSC+adiabatic cooling, respectively. In the second group, letter A denotes that the shell is moving at an increasing Lorentz factor, and s here describes the index of bulk acceleration law. In the third group, the letter G means that a broken power-law profile of 
is considered, while the acceleration effect is also taken into account (letter A). The index g describes the evolution of 
, which could refer to Eq. (5).
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