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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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