2016ApJS..225...17J


Query : 2016ApJS..225...17J

2016ApJS..225...17J - Astrophys. J., Suppl. Ser., 225, 17-17 (2016/July-0)

A statistical study of GRB X-ray flares: evidence of ubiquitous bulk acceleration in the emission region.

JIA L.-W., UHM Z.L. and ZHANG B.

Abstract (from CDS):

When emission in a conical relativistic jet ceases abruptly (or decays sharply), the observed decay light curve is controlled by the high-latitude "curvature effect." Recently, Uhm & Zhang found that the decay slopes of three gamma-ray burst (GRB) X-ray flares are steeper than what the standard model predicts. This requires bulk acceleration of the emission region, which is consistent with a Poynting-flux-dominated outflow. In this paper, we systematically analyze a sample of 85 bright X-ray flares detected in 63 Swift GRBs and investigate the relationship between the temporal decay index α and spectral index β during the steep decay phase of these flares. The α values depend on the choice of the zero time point t_0. We adopt two methods. "Method I" takes {t}_{0}^{I} as the first rising data point of each flare and is the most conservative approach. We find that at the 99.9% confidence level 56/85 flares have decay slopes steeper than the simplest curvature effect prediction and therefore are in the acceleration regime. "Method II" extrapolates the rising light curve of each flare backward until the flux density is three orders of magnitude lower than the peak flux density, and it defines the corresponding time as the zero time point ({t}_{0}^{II}). We find that 74/85 flares fall into the acceleration regime at the 99.9% confidence level. This suggests that bulk acceleration is common and may even be ubiquitous among X-ray flares, pointing toward a Poynting-flux-dominated jet composition for these events.

Abstract Copyright: © 2016. The American Astronomical Society. All rights reserved.

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

Simbad objects: 63

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Number of rows : 63
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 Fermi bn100802240 gB 00 09 52.47 +47 45 19.1           ~ 61 0
2 GRB 071031 gB 00 25 37.40 -58 03 33.9           ~ 184 0
3 Fermi bn090621185 gB 00 43 56.80 +61 56 17.6           ~ 59 0
4 GRB 100901A gB 01 49 03.56 +22 45 30.6           ~ 170 0
5 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
6 Fermi bn130925164 gB 02 44 42.38 -26 09 15.8           ~ 184 0
7 GRB 060312 gB 03 03 05.920 +12 50 02.00           ~ 50 0
8 GRB 100902A gB 03 14 30 +30 58.2           ~ 68 0
9 GRB 050822 gB 03 24 27.240 -46 01 59.20     20.82     ~ 115 0
10 Fermi bn130609902 gB 03 35 05.11 -40 10 26.7           ~ 54 0
11 Fermi bn091221870 gB 03 43 11.40 +23 14 28.0           ~ 66 0
12 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 275 0
13 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 208 0
14 GRB 090407 gB 04 35 54.98 -12 40 45.5           ~ 87 0
15 GRB 121108A gB 05 32 46.58 +54 28 24.7           ~ 39 0
16 Fermi bn100619015 gB 05 38 28.0 -27 00 02           ~ 57 0
17 GRB 110801A gB 05 57 44.87 +80 57 21.1           ~ 90 0
18 Fermi bn080928628 gB 06 20 16.85 -55 11 59.3           ~ 187 0
19 GRB 090904A gB 06 43 32.35 +50 12 10.8           ~ 43 0
20 GRB 140430A gB 06 51 44.58 +23 01 25.5           ~ 81 0
21 GRB 070520B gB 08 07 31.070 +57 36 30.00           ~ 42 0
22 GRB 140817A gB 08 29 03.35 +58 11 24.1           ~ 29 0
23 GRB 141031A gB 08 34 25.96 -59 10 05.8           ~ 34 0
24 Fermi bn100704149 gB 08 54 33.92 -24 12 09.7           ~ 103 0
25 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
26 GRB 050502B gB 09 30 10.024 +16 59 48.07           ~ 169 0
27 Fermi bn140206304 gB 09 41 16.90 +66 45 42.7           ~ 149 0
28 Fermi bn100727238 gB 10 16 42.67 -21 23 25.1           ~ 43 0
29 GRB 130131A gB 11 24 30.29 +48 04 33.2           ~ 42 0
30 GRB 121229A gB 12 40 23.41 -50 35 37.2           ~ 57 0
31 GRB 100302A gB 13 02 03.66 +74 35 22.5           ~ 83 0
32 GRB 091130B gB 13 32 35.62 +34 05 18.8           ~ 39 0
33 GRB 090417B gB 13 58 44.8 +47 00 55           ~ 119 1
34 GRB 060204B gB 14 07 14.900 +27 40 36.40           ~ 93 0
35 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 214 0
36 GRB 060814 gB 14 45 21.480 +20 35 11.80           ~ 241 0
37 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
38 GRB 080229 gB 15 12 52.31 -14 42 16.2           ~ 68 0
39 GRB 100526A gB 15 23 04.60 +25 37 55.9           ~ 35 0
40 GRB 080212 gB 15 24 35.400 -22 44 29.50           ~ 58 0
41 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
42 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
43 Fermi bn110102788 gB 16 23 31.41 +07 36 49.8           ~ 62 0
44 GRB 060929 gB 17 32 28.920 +29 50 06.20           ~ 60 0
45 GRB 090807 gB 18 14 57.80 +10 16 45.9           ~ 38 0
46 GRB 060111A gB 18 24 49.132 +37 36 14.47     18.86     ~ 72 0
47 Fermi bn140506880 gB 18 27 06.04 -55 38 08.7           ~ 113 0
48 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
49 Fermi bn140512814 gB 19 17 28.81 -15 05 39.5           ~ 133 0
50 Fermi bn100725475 gB 19 20 07 +76 57.3           ~ 55 0
51 GRB 130514A gB 19 45 07.33 -07 58 41.1           ~ 82 0
52 Fermi bn140709051 gB 20 18 38.96 +51 13 29.9           ~ 43 0
53 GRB 080805 gB 20 56 55.30 -62 25 58.8           ~ 102 0
54 GRB 050713A gB 21 22 09.530 +77 04 29.50           ~ 125 0
55 Fermi bn140108721 gB 21 40 26.77 +58 44 41.4           ~ 58 0
56 GRB 080506 gB 21 57 41.79 +38 59 06.7           ~ 46 0
57 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
58 GRB 060604 gB 22 28 55.010 -10 54 55.80 20.34 20.31       ~ 134 0
59 GRB 071021 gB 22 42 34.33 +23 43 05.4           ~ 104 0
60 GRB 110820A gB 22 52 46.10 +70 17 55.3           ~ 39 0
61 GRB 131030A gB 23 00 16.14 -05 22 05.2           ~ 126 0
62 GRB 090812 gB 23 32 48.5 -10 36 17           ~ 165 0
63 Fermi bn080810549 gB 23 47 08.00 +00 18 35.1           ~ 240 0

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