2018ApJ...859..160W


Query : 2018ApJ...859..160W

2018ApJ...859..160W - Astrophys. J., 859, 160-160 (2018/June-1)

Gamma-ray Burst jet breaks revisited.

WANG X.-G., ZHANG B., LIANG E.-W., LU R.-J., LIN D.-B., LI J. and LI L.

Abstract (from CDS):

Gamma-ray Burst (GRB) collimation has been inferred with the observations of achromatic steepening in GRB light curves, known as jet breaks. Identifying a jet break from a GRB afterglow light curve allows a measurement of the jet opening angle and true energetics of GRBs. In this paper, we re-investigate this problem using a large sample of GRBs that have an optical jet break that is consistent with being achromatic in the X-ray band. Our sample includes 99 GRBs from 1997 February to 2015 March that have optical and, for Swift GRBs, X-ray light curves that are consistent with the jet break interpretation. Out of the 99 GRBs we have studied, 55 GRBs are found to have temporal and spectral behaviors both before and after the break, consistent with the theoretical predictions of the jet break models, respectively. These include 53 long/soft (Type II) and 2 short/hard (Type I) GRBs. Only 1 GRB is classified as the candidate of a jet break with energy injection. Another 41 and 3 GRBs are classified as the candidates with the lower and upper limits of the jet break time, respectively. Most jet breaks occur at 90 ks, with a typical opening angle θj = (2.5 ± 1.0)°. This gives a typical beaming correction factor fb–1∼1000 for Type II GRBs, suggesting an even higher total GRB event rate density in the universe. Both isotropic and jet-corrected energies have a wide span in their distributions: log(Eγ,iso/erg) = 53.11 with σ = 0.84; log(EK,iso/erg) = 54.82 with σ = 0.56; log(Eγ/erg) = 49.54 with σ = 1.29; and log(EK/erg) = 51.33 with σ = 0.58. We also investigate several empirical correlations (Amati, Frail, Ghirlanda, and Liang-Zhang) previously discussed in the literature. We find that in general most of these relations are less tight than before. The existence of early jet breaks and hence small opening angle jets, which were detected in the Swfit era, is most likely the source of scatter. If one limits the sample to jet breaks later than 104 s, the Liang-Zhang relation remains tight and the Ghirlanda relation still exists. These relations are derived from Type II GRBs, and Type I GRBs usually deviate from them.

Abstract Copyright: © 2018. The American Astronomical Society.

Journal keyword(s): gamma-rays bursts: general - methods: statistical - radiation mechanisms: non-thermal

Simbad objects: 99

goto Full paper

goto View the references in ADS

Number of rows : 99
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 021004 gB 00 26 54.68 +18 55 41.6           ~ 547 0
6 GRB 080710 gB 00 33 05.68 +19 30 05.8           ~ 122 0
7 Fermi bn120729456 gB 00 52 17.84 +49 56 23.1           ~ 96 0
8 GRB 051028 gB 01 48 15.010 +47 45 09.20           ~ 38 0
9 GRB 100901A gB 01 49 03.56 +22 45 30.6           ~ 153 0
10 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 199 0
11 GRB 110918A gB 02 10 09.39 -27 06 19.6           ~ 77 0
12 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 273 1
13 GRB 071112C gB 02 36 50.89 +28 22 16.9           ~ 148 0
14 GRB 050603 gB 02 39 56.839 -25 10 54.92     18.48     ~ 165 0
15 GRB 060906 gB 02 43 00.900 +30 21 42.12     19.84     ~ 132 0
16 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 289 1
17 GRB 070318 gB 03 13 56.830 -42 56 46.30 18.27 16.23 15.49     ~ 156 0
18 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 253 0
19 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 192 0
20 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 147 0
21 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 193 0
22 Fermi bn101024486 gB 04 26 01.24 -77 15 55.1           ~ 49 0
23 GRB 991216 gB 05 09 31.2983 +11 17 07.262           ~ 421 0
24 GRB 061126 gB 05 46 24.460 +64 12 38.49 18.62 18.79 19.20     ~ 173 1
25 GRB 070311 gB 05 50 08.220 +03 22 29.40           ~ 65 0
26 GRB 090328 gB 06 02 39.69 -41 52 55.1           ~ 171 1
27 Fermi bn120711115 gB 06 18 42.839 -70 59 56.78           ~ 104 0
28 Fermi bn080928628 gB 06 20 16.85 -55 11 59.3           ~ 165 0
29 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 282 0
30 GRB 070411 gB 07 09 19.930 +01 03 52.60     17.94     ~ 127 0
31 GRB 070125 gB 07 51 17.80 +31 09 04.8           ~ 181 0
32 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 221 0
33 GRB 020124 gB 09 32 50.8 -11 31 11           ~ 152 0
34 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 206 1
35 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 258 0
36 GRB 100219A gB 10 16 48.48 -12 34 00.0           ~ 112 0
37 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1208 1
38 GRB 110205A gB 10 58 31.12 +67 31 31.2           ~ 185 0
39 GRB 030323 gB 11 06 09.4 -21 46 13           ~ 134 1
40 GRB 011211 gB 11 15 16 -21 56.0           ~ 299 0
41 GRB 130603B gB 11 28 48.16 +17 04 18.2           ~ 346 0
42 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 514 1
43 GRB 030226 gB 11 33 04.9 +25 53 56           ~ 204 0
44 GRB 050408 gB 12 02 17.320 +10 51 10.00           ~ 151 0
45 GRB 070419A gB 12 10 58.830 +39 55 34.06 18.52         ~ 118 0
46 GRB 030429 gB 12 13 07.495 -20 54 49.54     23.70     ~ 131 0
47 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 283 1
48 GRB 090426 gB 12 36 19.49 +32 59 05.5           ~ 205 0
49 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 220 1
50 GRB 060512 gB 13 03 05.810 +41 11 27.21 19.12 19.63 17.20     ~ 134 0
51 GRB 050502A gB 13 29 46.250 +42 40 27.50           ~ 63 0
52 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 313 0
53 GRB 050801 gB 13 36 35.000 -21 55 41.00 15.03 15.82 15.46     ~ 156 0
54 GRB 990510 gB 13 38 07.64 -80 29 48.8           ~ 488 1
55 GRB 080319A gB 13 45 19.97 +44 04 49.1           ~ 76 0
56 GRB 020405 gB 13 58 03.12 -31 22 22.2   21.9 21.5     ~ 249 1
57 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 313 0
58 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 467 0
59 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 189 0
60 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 164 0
61 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 192 0
62 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 989 1
63 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 269 0
64 GRB 081203A gB 15 32 07.6 +63 31 15           ~ 157 0
65 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 360 0
66 GRB 000301C gB 16 20 18.5 +29 26 35           ~ 356 0
67 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 335 0
68 GRB 050721 gB 16 53 44.530 -28 22 51.80     19.63     ~ 61 0
69 GRB 070518 gB 16 56 47.750 +55 17 41.40 18.68 19.22 19.01     ~ 70 0
70 GRB 000926 gB 17 04 15 +51 46.0           ~ 364 0
71 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 180 0
72 GRB 080319C gB 17 15 55.48 +55 23 31.7           ~ 157 0
73 Fermi bn120326056 gB 18 15 37.06 +69 15 35.4           ~ 158 0
74 GRB 120815A gB 18 15 54.40 -52 07 29.0           ~ 85 0
75 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 382 1
76 GRB 080603A gB 18 37 37.95 +62 44 39.6           ~ 82 0
77 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 197 0
78 GRB 060111B gB 19 05 42.480 +70 22 33.60     17.55     ~ 85 1
79 GRB 080413A gB 19 09 11.73 -27 40 39.6           ~ 143 0
80 GRB 071010A gB 19 12 14.42 -32 24 06.2           ~ 124 0
81 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 320 0
82 GRB 020813A gB 19 46 41.874 -19 36 04.81           ~ 303 0
83 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 170 0
84 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 282 0
85 GRB 060605 gB 21 28 37.320 -06 03 31.30   20.12 16.53     ~ 193 0
86 GRB 080413B gB 21 44 34.62 -19 58 51.2           ~ 168 0
87 GRB 030723 gB 21 49 24.40 -27 42 47.4           ~ 126 0
88 Fermi bn080804972 gB 21 54 41.90 -53 11 20.2           ~ 137 0
89 GRB 051221 gB 21 54 48.626 +16 53 27.16 19.49         ~ 351 1
90 GRB 060927A gB 21 58 11.930 +05 21 50.32           ~ 196 0
91 GRB 051109A gB 22 01 15.320 +40 49 23.70   20.09 20.14     ~ 173 0
92 GRB 090510 gB 22 14 12.60 -26 35 51.1           ~ 494 1
93 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 386 0
94 GRB 990712 gB 22 31 53.061 -73 24 28.58           ~ 262 1
95 GRB 051111A gB 23 12 33.170 +18 22 28.80 19.77 20.08 19.50     ~ 206 0
96 GRB 090812 gB 23 32 48.5 -10 36 17           ~ 143 0
97 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 303 0
98 GRB 071025 gB 23 40 17.02 +31 46 42.4           ~ 110 0
99 GRB 980703 gB 23 59 06.7 +08 35 07           ~ 445 1

To bookmark this query, right click on this link: simbad:objects in 2018ApJ...859..160W and select 'bookmark this link' or equivalent in the popup menu