2015ApJ...810..160G


Query : 2015ApJ...810..160G

2015ApJ...810..160G - Astrophys. J., 810, 160 (2015/September-2)

A morphological analysis of gamma-ray burst early-optical afterglows.

GAO H., WANG X.-G., MESZAROS P. and ZHANG B.

Abstract (from CDS):

Within the framework of the external shock model of gamma-ray burst (GRB) afterglows, we perform a morphological analysis of the early-optical light curves to directly constrain model parameters. We define four morphological types, i.e., the reverse shock-dominated cases with/without the emergence of the forward shock peak (Type I/Type II), and the forward shock-dominated cases without/with νm crossing the band (Type III/IV). We systematically investigate all of the Swift GRBs that have optical detection earlier than 500 s and find 3/63 Type I bursts (4.8%), 12/63 Type II bursts (19.0%), 30/63 Type III bursts (47.6%), 8/63 Type IV bursts (12.7%), and 10/63 Type III/IV bursts (15.9%). We perform Monte Carlo simulations to constrain model parameters in order to reproduce the observations. We find that the favored value of the magnetic equipartition parameter in the forward shock (εBf) ranges from 10–6 to 10–2, and the reverse-to-forward ratio of ∈B(RB) is about 100. The preferred electron equipartition parameter εer,f value is 0.01, which is smaller than the commonly assumed value, e.g., 0.1. This could mitigate the so-called ''efficiency problem'' for the internal shock model, if ∈e during the prompt emission phase (in the internal shocks) is large (say, ∼0.1). The preferred RB value is in agreement with the results in previous works that indicate a moderately magnetized baryonic jet for GRBs.

Abstract Copyright: ∼

Journal keyword(s): gamma-ray burst: general

Simbad objects: 64

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Number of rows : 64
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 GRB 070611 gB 00 07 58.000 -29 45 19.40           ~ 94 0
2 GRB 071031 gB 00 25 37.40 -58 03 33.9           ~ 184 0
3 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
4 GRB 080710 gB 00 33 05.68 +19 30 05.8           ~ 136 0
5 GRB 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
6 GRB 100901A gB 01 49 03.56 +22 45 30.6           ~ 170 0
7 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
8 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
9 GRB 071112C gB 02 36 50.89 +28 22 16.9           ~ 164 0
10 GRB 060906 gB 02 43 00.900 +30 21 42.12     19.84     ~ 147 0
11 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
12 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 315 1
13 GRB 070318 gB 03 13 56.830 -42 56 46.30 18.27 16.23 15.49     ~ 170 0
14 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
15 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 275 0
16 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 208 0
17 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 168 0
18 GRB 060110 gB 04 50 57.850 +28 25 55.70           ~ 59 0
19 GRB 970228 gB 05 01 46.7 +11 46 53           ~ 650 1
20 GRB 061126 gB 05 46 24.460 +64 12 38.49 18.62 18.79 19.20     ~ 182 1
21 Fermi bn120711115 gB 06 18 42.839 -70 59 56.78           ~ 125 0
22 Fermi bn080928628 gB 06 20 16.85 -55 11 59.3           ~ 187 0
23 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
24 GRB 070411 gB 07 09 19.930 +01 03 52.60     17.94     ~ 138 0
25 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 193 0
26 GRB 070420 gB 08 04 55.170 -45 33 19.99 20.39 20.01 17.16     ~ 83 0
27 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
28 GRB 071010B gB 10 02 09.20 +45 43 52.2           ~ 173 0
29 Fermi bn121217313 gB 10 14 50.32 -62 21 03.3           ~ 69 0
30 GRB 100219A gB 10 16 48.48 -12 34 00.0           ~ 130 0
31 GRB 030418 gB 10 54 33.69 -07 01 40.8           ~ 69 0
32 GRB 110205A gB 10 58 31.12 +67 31 31.2           ~ 213 0
33 GRB 080330 gB 11 17 06.70 +30 36 24.1           ~ 145 0
34 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
35 GRB 011121 gB 11 34 26.67 -76 01 41.6       23.0   ~ 286 1
36 GRB 070419A gB 12 10 58.830 +39 55 34.06 18.52         ~ 130 0
37 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
38 GRB 090313 gB 13 13 36.00 +08 05 10.7           ~ 149 0
39 GRB 080319A gB 13 45 19.97 +44 04 49.1           ~ 79 0
40 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
41 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 1012 1
42 GRB 081203A gB 15 32 07.6 +63 31 15           ~ 177 0
43 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
44 GRB 090726 gB 16 34 43.50 +72 51 56.5           ~ 70 0
45 GRB 080319C gB 17 15 55.48 +55 23 31.7           ~ 174 0
46 GRB 060926 gB 17 35 43.660 +13 02 18.60     19.36     ~ 135 0
47 GRB 120815A gB 18 15 54.40 -52 07 29.0           ~ 103 0
48 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
49 GRB 080603A gB 18 37 37.95 +62 44 39.6           ~ 89 0
50 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
51 GRB 060111B gB 19 05 42.480 +70 22 33.60     17.55     ~ 92 1
52 GRB 071010A gB 19 12 14.42 -32 24 06.2           ~ 138 0
53 GRB 060605 gB 21 28 37.320 -06 03 31.30   20.12 16.53     ~ 210 0
54 Fermi bn081126899 gB 21 34 03.54 +48 42 35.2           ~ 76 0
55 GRB 060117 gB 21 51 36.130 -59 58 39.10           ~ 63 0
56 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
57 Fermi bn081109293 gB 22 03 11.50 -54 42 40.5           ~ 125 1
58 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
59 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
60 Fermi bn091024380 gB 22 37 +56.9           ~ 151 0
61 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1
62 GRB 090812 gB 23 32 48.5 -10 36 17           ~ 165 0
63 GRB 071025 gB 23 40 17.02 +31 46 42.4           ~ 122 0
64 Fermi bn080810549 gB 23 47 08.00 +00 18 35.1           ~ 240 0

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