Table A.1.
Best-fit parameters of the simple (PL) and broken power-law (BPL) models for all the 40 SGRBs light curves in the LC fit sample (see Sect. 3.1).
GRB name | z | t0 | α1 | α2 | tbreak | Fpl, norm/break | χ2 | ν | p-value |
---|---|---|---|---|---|---|---|---|---|
(s) | (×103 s) | (×10−12 erg cm−2 s−1) | |||||||
050724(F) | 0.254 | 370 | 0.93 ± 0.06 | - | - | (1.63 ± 0.19) | 23.9 | 10 | 1.0 |
061006 | 0.461 | 168 | 0.78 ± 0.05 | - | - | (1.45 ± 0.13) | 13.3 | 9 | 1.0 |
070724A | 0.457 | 385 | 1.16 ± 0.10 | - | - | (1.3 ± 0.3) | 21.8 | 4 | 8.58 × 10−2 |
070809 | 0.2187 | 126 | 0.50 ± 0.06 | - | - | (1.7 ± 0.2) | 43.0 | 14 | 1.14 × 10−3 |
090426 | 2.609 | 120 | 0.95 ± 0.03 | - | - | (2.85 ± 0.19) | 40.9 | 25 | 7.57 × 10−3 |
111117A | 2.211 | 200 | 1.22 ± 0.07 | - | - | (5.4 ± 0.6)×10−1 | 4.8 | 5 | 7.99 × 10−1 |
120804A | 1.05 | 150 | 1.08 ± 0.03 | - | - | (1.26 ± 0.07)×10 | 55.1 | 30 | 1.0 |
121226A | 1.37 | 146 | 0.97 ± 0.05 | - | - | (5.0 ± 0.5) | 21.5 | 11 | 1.36 × 10−1 |
131004A(F) | 0.717 | 105 | 1.00 ± 0.06 | - | - | (4.9 ± 0.7) | 25.5 | 8 | 1.60 × 10−1 |
140129B | 0.43 | 400 | 1.29 ± 0.09 | - | - | (5.9 ± 0.8) | 24.0 | 15 | 1.52 × 10−2 |
140930B | 1.465 | 214 | 1.75 ± 0.10 | - | - | (1.4 ± 0.2) | 61.7 | 23 | 1.0 |
150423A | 1.394 | 100 | 0.91 ± 0.06 | - | - | (1.11 ± 0.13) | 4.5 | 6 | 6.47 × 10−2 |
150831A | 1.18 | 200 | 1.07 ± 0.08 | - | - | (0.71 ± 0.10) | 2.2 | 4 | 1.0 |
160303A | 1.01 | 600 | 0.68 ± 0.10 | - | - | (0.76 ± 0.13) | 15.2 | 5 | 2.90 × 10−1 |
160525B | 0.64 | 99 | 1.35 ± 0.10 | - | - | (0.67 ± 0.14) | 27.4 | 11 | 1.0 |
160821B | 0.1619 | 300 | 1.33 ± 0.13 | - | - | (2.0 ± 0.6) | 16.2 | 3 | 7.94 × 10−1 |
170728A | 1.493 | 250 | 0.98 ± 0.07 | - | - | (3.6 ± 0.4) | 5.9 | 4 | 4.76 × 10−1 |
180418A | 1.56 | 3170 | 0.84 ± 0.04 | - | - | (2.2 ± 0.15) | 17.8 | 16 | 1.0 |
180727A | 1.95 | 100 | 1.20 ± 0.09 | - | - | (0.9 ± 0.2) | 6.1 | 3 | 1.0 |
180805B | 0.6612 | 479 | 1.16 ± 0.11 | - | - | (1.3 ± 0.2) | 16.3 | 8 | 1.0 |
191019A | 0.248 | 3545 | 1.13 ± 0.13 | - | - | (1.22 ± 0.13) | 9.1 | 6 | 8.19 × 10−2 |
200411A | 0.82 | 400 | 0.84 ± 0.08 | - | - | (2.0 ± 0.2) | 18.7 | 9 | 1.0 |
200522A | 0.5536 | 450 | 0.64 ± 0.08 | - | - | (1.3 ± 0.2) | 6.6 | 3 | 7.40 × 10−1 |
210726A | 0.37 | 500 | 0.56 ± 0.02 | - | - | (1.41 ± 0.08) | 2.5 | 7 | 9.90 × 10−1 |
211023B | 0.862 | 750 | 0.78 ± 0.06 | - | - | (1.48 ± 0.15) | 8.9 | 6 | 1.0 |
051221A | 0.5464 | 314 | 0.65 ± 0.03 | 1.44 ± 0.08 | 6.16 × 10 | (5.5 ± 0.4)×10−1 | 96.6 | 60 | 1.26 × 10−8 |
060614 | 0.125 | 4000 | 0.06 ± 0.03 | 1.81 ± 0.03 | 4.45 × 10 | (5.8 ± 0.2) | 172.9 | 149 | 1.11 × 10−16 |
061201 | 0.111 | 80 | 0.65 ± 0.06 | 2.12 ± 0.10 | 3.00 | (3.9 ± 0.5)×10 | 29.3 | 24 | 2.50 × 10−9 |
070714B | 0.923 | 300 | 0.65 ± 0.12 | 2.11 ± 0.10 | 2.13 | (1.8 ± 0.2)×10 | 44.8 | 25 | 2.43 × 10−6 |
090510 | 0.903 | 100 | 0.66 ± 0.03 | 2.28 ± 0.06 | 1.67 | (7.6 ± 0.4)×10 | 93.4 | 99 | 1.11 × 10−16 |
110402A | 0.854 | 593 | 0.48 ± 0.06 | 2.25 ± 0.15 | 8.43 | (2.0 ± 0.2) | 13.7 | 15 | 6.11 × 10−6 |
130603B | 0.3568 | 70 | 0.38 ± 0.03 | 1.69 ± 0.06 | 2.90 | (3.3 ± 0.2)×10 | 128.8 | 69 | 1.11 × 10−16 |
140903A | 0.3529 | 200 | 0.15 ± 0.03 | 1.25 ± 0.05 | 9.65 | (9.7 ± 0.5) | 28.2 | 34 | 8.55 × 10−15 |
150424A | 0.3 | 453 | 0.76 ± 0.02 | 2.4 ± 0.3 | 2.03 × 102 | (3.9 ± 0.3)×10−1 | 23.3 | 32 | 1.24 × 10−6 |
151229A | 0.63 | 90 | 0.26 ± 0.19 | 0.96 ± 0.04 | 3.47 × 10−1 | (2.8 ± 0.9)×102 | 73.1 | 70 | 9.51 × 10−7 |
161001A | 0.67 | 207 | 0.75 ± 0.05 | 1.37 ± 0.05 | 3.53 | (4.9 ± 0.4)×10 | 57.3 | 45 | 1.45 × 10−5 |
170728B | 1.272 | 400 | 0.53 ± 0.03 | 1.34 ± 0.02 | 2.53 | (2.1 ± 0.1)×102 | 213.6 | 193 | 1.11 × 10−16 |
180618A | 0.52 | 80 | 0.11 ± 0.40 | 1.77 ± 0.04 | 1.27 × 10−1 | (1.8 ± 0.2) | 130.4 | 97 | 2.98 × 10−11 |
210323A | 0.733 | 800 | 0.50 ± 0.06 | 3.4 ± 0.3 | 1.32 × 10 | (4.2 ± 0.4) | 10.4 | 10 | 1.22 × 10−5 |
211211A | 0.0763 | 3400 | −0.12 ± 0.18 | 2.07 ± 0.08 | 7.97 | (5.5 ± 0.6)×10 | 72.9 | 47 | 2.39 × 10−10 |
Notes. The first 25 bursts are the ones for which a power-law model was enough to describe the light curve behaviour (PL subsample). The last 15 bursts are the BPL subsample, for which the addition of a break resulted statistically significant (see Sec. 3.2). The (F) marks the cases for which a flaring component was discarded to allow a better fit of the afterglow.
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