Table C.1
Light curve models and parameters used to flux normalize XRT X-ray and GROND NIR/optical data to a common reference time.
Model | α 1 | α 2 | α 3 | t break | Host | Additional dataa | |
(ks) | (y/n) | (reference) | |||||
|
|||||||
GRB 071025 | |||||||
NIR/opt. | PL | 1.32 ± 0.11 | ... | ... | ... | no | PAIRTEL JHKs (1) |
X-ray | PL | 1.60 ± 0.01 | ... | ... | ... | ||
|
|||||||
GRB 080825Bb | |||||||
NIR/opt. | BRPL | 1.1 ± 0.1 | 2.2 ± 0.6 | ... | 59 ± 24 | no | DFOSC I(2) |
X-ray | PL | 1.8 ± 0.6 | ... | ... | ... | ||
|
|||||||
GRB 080913 | |||||||
NIR/opt. | PL | 1.13 ± 0.08 | ... | ... | ... | no | |
X-ray | PL | 1.22 ± 0.06 | ... | ... | ... | ||
|
|||||||
GRB 080916C | |||||||
NIR/opt. | PL | 1.73 ± 0.39 | ... | ... | ... | no | |
X-ray | PL | 1.30 ± 0.09 | ... | ... | ... | ||
|
|||||||
GRB 090205 | |||||||
NIR/opt. | PL | 1.35 ± 0.04 | ... | ... | ... | yes | FORS1 RI (3) |
X-ray | BRPL | 0.91 ± 0.03 | 2.12 ± 0.07 | ... | 23 ± 1 | ||
|
|||||||
GRB 090423 | |||||||
NIR/opt. | BRPL | 0.05 ± 0.01 | 1.00 ± 0.03 | ... | 24 ± 8 | no | HAWKI KJ/WFCAM K |
X-ray | PL + BRPL | 1.38 ± 0.04 | −3.75 ± 4.20 | 1.34 ± 0.15 | 3.0 ± 4.6 | NIRI HJ/ISAAK J (4)(5) | |
|
|||||||
GRB 090429Bc | |||||||
NIR/opt. | PL | 0.61 ± 0.08 | ... | ... | ... | no | NIRI JHK (6) |
X-ray | BRPL | −1.14 ± 0.59 | 1.37 ± 0.10 | ... | 0.65 ± 0.18 | ||
|
|||||||
GRB 090516A | |||||||
NIR/opt. | PL | 1.72 ± 0.05 | ... | ... | ... | yes | FORS2 R (7)/NOT R (8) |
X-ray | BRPL | 0.78 ± 0.06 | 1.75 ± 0.05 | ... | 16 ± 1 | ||
|
|||||||
GRB 100219A | |||||||
NIR/opt. | PL | 1.68 ± 0.46 | ... | ... | ... | yes | HAWKI KHJ/GMG r′ |
X-ray | BRPL | 1.72 ± 0.25 | > 3.0 | ... | ... | GTC i′ (9) | |
|
|||||||
GRB 100513A | |||||||
NIR/opt. | PL | 0.48 ± 0.17 | ... | ... | ... | no | PAIRITEL JHKs (10) |
X-ray | PL | 0.96 ± 0.06 | ... | ... | ... | ||
GRB 100905A | |||||||
NIR/opt. | PL | 0.60 ± 0.06 | ... | ... | ... | no | |
X-ray | PL | 0.88 ± 0.03 | ... | ... | ... | ||
|
|||||||
GRB 111008A | |||||||
NIR/opt. | PL | 1.02 ± 0.06 | ... | ... | ... | no | |
X-ray | BRPL | 0.97 ± 0.09 | 1.42 ± 0.05 | ... | 41 ± 11 | ||
|
|||||||
GRB 120712A | |||||||
NIR/opt. | BRPL | 0.04 ± 0.08 | 1.66 ± 0.16 | ... | 102 ± 13 | no | |
X-ray | BRPL | 0.95 ± 0.03 | 1.80 ± 0.11 | ... | 6 ± 1 | ||
|
|||||||
GRB 130606A | |||||||
NIR/opt. | PL | 1.71 ± 0.03 | ... | ... | ... | no | NOT r′i′z′/TNG i′z′ (11) |
X-ray | PL | 1.71 ± 0.03 | ... | ... | ... | GTC i′z′ (12) | |
|
|||||||
GRB 131117A | |||||||
NIR/opt. | PL | 0.86 ± 0.01 | ... | ... | ... | no | |
X-ray | PL + G | 0.95 ± 0.02 | ... | ... | ... | ||
|
|||||||
GRB 140304A | |||||||
NIR/opt. | PL + BRPL | 2.25 ± 0.24 | −7.42 ± 5.94 | 1.86 ± 0.20 | 25 ± 2 | no | RATIR grizJH (13) |
X-ray | PL + BRPL | 1.93 ± 0.14 | −9.71 ± 6.89 | 1.50 ± 0.09 | 16 ± 2 | Nanshan R (14)/NOT gr (15) | |
MONDY R(16)/ORI-40 R (17) | |||||||
|
|||||||
GRB 140311A | |||||||
NIR/opt. | PL | 0.95 ± 0.04 | ... | ... | ... | no | NOT r′i′ (18) |
X-ray | BRPL | 1.20 ± 0.07 | 1.97 ± 0.58 | ... | 121 ± 65 | ||
|
|||||||
GRB 140428A | |||||||
NIR/opt. | PL | 1.81 ± 0.08 | ... | ... | ... | no | OSN I (19) |
X-ray | BRPL | 0.96 ± 0.07 | > 2.0 | ... | 19 ± 9 | LRIS i (20) | |
|
|||||||
GRB 140515A | |||||||
NIR/opt. | BRPL | 0.77 ± 0.25 | > 2.5 | ... | ... | no | GMOS z′ (21) |
X-ray | PL + BRPL | 3.10 ± 0.19 | −3.77 ± 0.69 | 1.03 ± 0.05 | 2.3 ± 0.2 | Chandra (22) | |
|
|||||||
GRB 140614A | |||||||
NIR/opt. | PL | 1.20 ± 0.04 | ... | ... | ... | no | |
X-ray | PL + BRPL | 1.92 ± 0.07 | −0.27 ± 0.32 | 1.49 ± 0.08 | 7 ± 1 | ||
|
|||||||
GRB 151027B | |||||||
NIR/opt. | BRPL | 0.44 ± 0.19 | 1.44 ± 0.14 | ... | 34 ± 28 | no | NOT R (23) |
X-ray | BRPL | 0.44 ± 0.19 | 1.44 ± 0.14 | ... | 34 ± 28 | RATIR r′i′ (24) | |
|
|||||||
GRB 151112A | |||||||
NIR/opt. | BRPL | 0.84 ± 0.06 | 2.10 ± 0.29 | ... | 128 ± 14 | no | |
X-ray | BRPL | 0.84 ± 0.06 | > 1.2 | ... | 128 ± 14 |
Notes.
GROND optical and near-infrared data were extended with data collected from GCNs and refereed publications. The magnitudes were, if necessary, converted to the AB system.
The XRT light curve is also consistent with the model for the NIR/optical afterglow (see Fig. B.2).
We used the temporal decay slope as derived from the NIRI K band data to re-scale the NIRI J, H, and K-band observation to a common reference time (see Fig. B.7).
Reference. (1) Perley et al. (2010); (2) Thoene et al. (2008); (3) D’Avanzo et al. (2010); (4) Tanvir et al. (2009); (5) Salvaterra et al. (2009); (6) Cucchiara et al. (2011); (7) Gorosabel et al. (2009); (8) de Ugarte Postigo et al. (2009); (9) Thöne et al. (2013); (10) Morgan et al. (2010); (11)Hartoog et al. (2015); (12) Castro-Tirado et al. (2013); (13) Butler et al. (2014); (14) Xu et al. (2014b); (15) de Ugarte Postigo et al. (2014); (16) Volnova et al. (2014a); (17) Volnova et al. (2014b); (18) Xu et al. (2014a); (19) Aceituno et al. (2014); (20) Perley (2014a); (21) Melandri et al. (2015); (22) Margutti et al. (2014); (23) Malesani et al. (2015b); (24) Watson et al. (2015a).
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