2015ApJS..219....9W


Query : 2015ApJS..219....9W

2015ApJS..219....9W - Astrophys. J., Suppl. Ser., 219, 9 (2015/July-0)

How bad or good are the external forward shock afterglow models of gamma-ray bursts?

WANG X.-G., ZHANG B., LIANG E.-W., GAO H., LI L., DENG C.-M., QIN S.-M., TANG Q.-W., KANN D.A., RYDE F. and KUMAR P.

Abstract (from CDS):

The external forward shock models have been the standard paradigm to interpret the broadband afterglow data of gamma-ray bursts (GRBs). One prediction of the models is that some afterglow temporal breaks at different energy bands should be achromatic; that is, the break times should be the same in different frequencies. Multiwavelength observations in the Swift era have revealed chromatic afterglow behaviors at least in some GRBs, casting doubts on the external forward shock origin of GRB afterglows. In this paper, using a large sample of GRBs with both X-ray and optical afterglow data, we perform a systematic study to address the question: how bad or good are the external forward shock models? Our sample includes 85 GRBs up to 2014 March with well-monitored X-ray and optical light curves. Based on how well the data abide by the external forward shock models, we categorize them into five grades and three samples. The first two grades (Grade I and II) include 45 of 85 GRBs. They show evidence of, or are consistent with having, an achromatic break. The temporal and spectral behaviors in each afterglow segment are consistent with the predictions (the ''closure relations'') of the forward shock models. These GRBs are included in the Gold sample. The next two grades (Grade III and IV) include 37 of 85 GRBs. They are also consistent with having an achromatic break, even though one or more afterglow segments do not comply with the closure relations. These GRBs are included in the Silver sample. Finally, Grade V (3/85) shows direct evidence of chromatic behaviors, suggesting that the external shock models are inconsistent with the data. These are included in the Bad sample. We further perform statistical analyses of various observational properties (temporal index α, spectral index β, break time tb) and model parameters (energy injection index q, electron spectral index p, jet opening angle, radiative efficiency ηγ, and so on) of the GRBs in the Gold sample, and derive constraints on the magnetization parameter ∈B in the forward shock. Overall, we conclude that the simplest external forward shock models can account for the multiwavelength afterglow data of at least half of the GRBs. When more advanced modeling (e.g., long-lasting reverse shock, structured jets, arbitrary circumburst medium density profile) is invoked, up to >90% of the afterglows may be interpreted within the framework of the external shock models.

Abstract Copyright:

Journal keyword(s): methods: statistical - gamma-ray burst: general - radiation mechanisms: nonthermal

Simbad objects: 85

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Number of rows : 85
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 GRB 070110 gB 00 03 39.270 -52 58 27.00 21.8 21.9 21.2     ~ 201 0
2 GRB 070611 gB 00 07 58.000 -29 45 19.40           ~ 89 0
3 GRB 060912A gB 00 21 08.11 +20 58 18.9           ~ 103 1
4 GRB 071031 gB 00 25 37.40 -58 03 33.9           ~ 166 0
5 GRB 080710 gB 00 33 05.68 +19 30 05.8           ~ 122 0
6 Fermi bn120729456 gB 00 52 17.84 +49 56 23.1           ~ 96 0
7 GRB 051028 gB 01 48 15.010 +47 45 09.20           ~ 38 0
8 GRB 100901A gB 01 49 03.56 +22 45 30.6           ~ 153 0
9 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 199 0
10 GRB 110918A gB 02 10 09.39 -27 06 19.6           ~ 77 0
11 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 273 1
12 GRB 071112C gB 02 36 50.89 +28 22 16.9           ~ 148 0
13 GRB 050603 gB 02 39 56.839 -25 10 54.92     18.48     ~ 165 0
14 GRB 060906 gB 02 43 00.900 +30 21 42.12     19.84     ~ 132 0
15 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 289 1
16 GRB 070318 gB 03 13 56.830 -42 56 46.30 18.27 16.23 15.49     ~ 156 0
17 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 253 0
18 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 192 0
19 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 147 0
20 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 193 0
21 Fermi bn101024486 gB 04 26 01.24 -77 15 55.1           ~ 49 0
22 GRB 061126 gB 05 46 24.460 +64 12 38.49 18.62 18.79 19.20     ~ 173 1
23 GRB 070311 gB 05 50 08.220 +03 22 29.40           ~ 65 0
24 GRB 090328 gB 06 02 39.69 -41 52 55.1           ~ 171 1
25 Fermi bn120711115 gB 06 18 42.839 -70 59 56.78           ~ 104 0
26 Fermi bn080928628 gB 06 20 16.85 -55 11 59.3           ~ 165 0
27 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 282 0
28 GRB 070411 gB 07 09 19.930 +01 03 52.60     17.94     ~ 127 0
29 GRB 070125 gB 07 51 17.80 +31 09 04.8           ~ 181 0
30 GRB 070420 gB 08 04 55.170 -45 33 19.99 20.39 20.01 17.16     ~ 80 0
31 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 221 0
32 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 206 1
33 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 258 0
34 GRB 100219A gB 10 16 48.48 -12 34 00.0           ~ 112 0
35 GRB 110205A gB 10 58 31.12 +67 31 31.2           ~ 185 0
36 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 516 1
37 GRB 050408 gB 12 02 17.320 +10 51 10.00           ~ 151 0
38 GRB 070419A gB 12 10 58.830 +39 55 34.06 18.52         ~ 118 0
39 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 283 1
40 GRB 090426 gB 12 36 19.49 +32 59 05.5           ~ 205 0
41 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 220 1
42 GRB 060512 gB 13 03 05.810 +41 11 27.21 19.12 19.63 17.20     ~ 134 0
43 GRB 070208 gB 13 11 32.607 +61 57 54.37 20.79 20.79 19.86     ~ 108 0
44 GRB 090313 gB 13 13 36.00 +08 05 10.7           ~ 137 0
45 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 313 0
46 GRB 050801 gB 13 36 35.000 -21 55 41.00 15.03 15.82 15.46     ~ 156 0
47 GRB 080319A gB 13 45 19.97 +44 04 49.1           ~ 76 0
48 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 313 0
49 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 467 0
50 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 189 0
51 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 164 0
52 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 192 0
53 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 269 0
54 GRB 081203A gB 15 32 07.6 +63 31 15           ~ 157 0
55 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 360 0
56 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 335 0
57 GRB 050721 gB 16 53 44.530 -28 22 51.80     19.63     ~ 61 0
58 GRB 070518 gB 16 56 47.750 +55 17 41.40 18.68 19.22 19.01     ~ 70 0
59 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 180 0
60 GRB 080319C gB 17 15 55.48 +55 23 31.7           ~ 157 0
61 Fermi bn120326056 gB 18 15 37.06 +69 15 35.4           ~ 158 0
62 GRB 120815A gB 18 15 54.40 -52 07 29.0           ~ 85 0
63 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 382 1
64 GRB 080603A gB 18 37 37.95 +62 44 39.6           ~ 82 0
65 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 197 0
66 GRB 060111B gB 19 05 42.480 +70 22 33.60     17.55     ~ 85 1
67 GRB 080413A gB 19 09 11.73 -27 40 39.6           ~ 143 0
68 GRB 071010A gB 19 12 14.42 -32 24 06.2           ~ 124 0
69 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 320 0
70 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 170 0
71 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 282 0
72 GRB 060614 gB 21 23 32.140 -53 01 36.10 18.89 20.12 19.54     ~ 614 1
73 GRB 060605 gB 21 28 37.320 -06 03 31.30   20.12 16.53     ~ 193 0
74 GRB 080413B gB 21 44 34.62 -19 58 51.2           ~ 168 0
75 Fermi bn080804972 gB 21 54 41.90 -53 11 20.2           ~ 137 0
76 GRB 051221 gB 21 54 48.626 +16 53 27.16 19.49         ~ 351 1
77 GRB 060927A gB 21 58 11.930 +05 21 50.32           ~ 196 0
78 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 295 0
79 GRB 051109A gB 22 01 15.320 +40 49 23.70   20.09 20.14     ~ 173 0
80 GRB 090510 gB 22 14 12.60 -26 35 51.1           ~ 494 1
81 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 386 0
82 GRB 051111A gB 23 12 33.170 +18 22 28.80 19.77 20.08 19.50     ~ 206 0
83 GRB 090812 gB 23 32 48.5 -10 36 17           ~ 143 0
84 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 303 0
85 GRB 071025 gB 23 40 17.02 +31 46 42.4           ~ 110 0

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