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Table 5

Time-resolved spectral analysis of the first episode in GRB 090618.

Time α β E0 (keV) kT (keV) γ kTLAD (keV) γLAD

A:0–5 –0.45  ±  0.11 –2.89  ±  0.78 208.9  ±  36.13 0.93 59.86  ±  2.72 1.62  ±  0.07 1.07 52.52  ±  23.63 1.42  ±  0.06 0.93
B:5–10 –0.16  ±  0.17 –2.34  ±  0.18 89.84  ±  17.69 1.14 37.57  ±  1.76 1.56  ±  0.05 1.36 37.39  ±  2.46 1.55  ±  0.06 1.27
C:10–17 –0.74  ±  0.08 –3.36  ±  1.34 149.7  ±  21.1 0.98 34.90  ±  1.63 1.72  ±  0.05 1.20 36.89  ±  2.40 1.75  ±  0.06 1.10
D:17–23 –0.51  ±  0.17 –2.56  ±  0.26 75.57  ±  16.35 1.11 25.47  ±  1.38 1.75  ±  0.06 1.19 25.70  ±  1.76 1.75  ±  0.08 1.19
E:23–31 –0.93  ±  0.13 unconstr. 104.7  ±  21.29 1.08 23.75  ±  1.68 1.93  ±  0.10 1.13 24.45  ±  2.24 1.95  ±  0.12 1.31
F:31–39 –1.27  ±  0.28 –3.20  ±  1.00 113.28  ±  64.7 1.17 18.44  ±  1.46 2.77  ±  0.83 1.10 18.69  ±  1.89 4.69  ±  4.2 1.08
G:39–49 –3.62  ±  1.00 –2.19  ±  0.17 57.48  ±  50.0 1.15 14.03  ±  2.35 3.20  ±  1.38 1.10 14.71  ±  3.52 3.06  ±  3.50 1.09

Notes. We considered seven time intervals and used two spectral models, whose best-fit parameters are shown here. The last three columns, marked with a LAD subscript, report the same analysis but in the energy range 20 − 1900 keV, which is the same energy range of the BATSE-LAD detector as used in the work of Ryde & Pe’er (2009).

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