Table 1
Time-resolved spectral analysis of GRB 090618.
Time interval | α | β | ![]() |
![]() |
γ | ![]() |
![]() |
|
|||||||
0–50 | –0.77![]() |
–2.33![]() |
128.12![]() |
1.11 | 0.91![]() |
180.9![]() |
1.13 |
50–57 | –0.93![]() |
–2.30 ± 0.10 | 104.98![]() |
1.22 | 1.11![]() |
168.3![]() |
1.22 |
57–68 | –0.93![]() |
–2.43![]() |
264.0![]() |
1.85 | 1.01![]() |
340.5![]() |
1.93 |
68–76 | –1.05![]() |
–2.49![]() |
243.9![]() |
1.88 | 1.12![]() |
311.0![]() |
1.90 |
76–103 | –1.06![]() |
–2.65![]() |
125.7![]() |
1.23 | 1.15![]() |
157.7![]() |
1.39 |
103–150 | –1.50![]() |
–2.30 ± 0.10 | 101.1![]() |
1.07 | 1.50![]() |
102.8![]() |
1.06 |
Notes. We considered six time intervals, each one corresponding to a particular emission feature in the light curve. We fitted the GBM (8 keV–10 MeV) observed emission with a Band model (Band et al. 1993) and a power-law function with an exponential cut-off. In Cols. 2 − 4 we list the Band model low-energy index α, the high-energy β and the break energy , with the reduced chi-square value in the 6th column. In the last three columns are listed the power-law index γ, the cut-off energy
and the reduced chi-square value respectively, as obtained from the spectral fit with the cut-off power-law spectral function.
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