2022ApJ...941...99L


Query : 2022ApJ...941...99L

2022ApJ...941...99L - Astrophys. J., 941, 99 (2022/December-2)

The Spectral Evolution Patterns and Implications of Gamma-Ray Burst X-Ray Flares.

LU L.-Z., LIANG E.-W. and CORDIER B.

Abstract (from CDS):

We present a time-resolved spectral analysis of bright X-ray flares observed by Swift X-ray telescope from 2004 December to 2021 December. We selected 58 bright flares from 56 gamma-ray burst X-ray afterglows to perform time-resolved spectral analysis. We find that there is a strong spectral evolution in X-ray flares. Spectral evolution exists in all the X-ray flares. We have not found flares without spectral evolutions in our samples. The spectrum of an X-ray afterglow is dominated by the flare when it exists. Four spectral evolution patterns were found, i.e., hard-to-soft, intensity tracking, soft-to-hard, and anti-intensity tracking. Most of the flares (46 flares, 79.3%) show a spectral evolution from hard to soft. Five (8.6%) flares are intensity tracking. Two (3.5%) flares show soft-to-hard. Five (8.6%) flares show anti-intensity tracking. Therefore, hard-to-soft spectral evolution patterns dominate the spectral evolutions of X-ray flares. In other words, the hard-to-soft spectral evolution pattern is the main evolution pattern of X-ray flares. Hard-to-soft, intensity tracking, and soft-to-hard spectral evolution patterns are the same as prompt emission spectral evolutions, indicating that the origin of flares should be the same as prompt emissions and the flares are the lower energy band emissions of the prompt emissions. The spectral evolution intensities are independent of the peak time and FWHM of the flares. In other words, the spectral evolution intensity is irrelevant to the flare occurrence time and its duration but related to the peak fluxes of flares. This means that the more luminous the flares, the stronger the spectral evolutions.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Light curves - Gamma-ray bursts - Spectral index

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 050908 gB 01 21 50.750 -12 57 17.20           ~ 179 0
5 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
6 GRB 070129 gB 02 28 00.940 +11 41 04.00       21.3   ~ 120 0
7 GRB 100902A gB 03 14 30 +30 58.2           ~ 68 0
8 GRB 050822 gB 03 24 27.240 -46 01 59.20     20.82     ~ 115 0
9 Fermi bn091221870 gB 03 43 11.40 +23 14 28.0           ~ 66 0
10 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 208 0
11 Fermi bn170113420 gB 04 06 59 -71 56.0           ~ 64 0
12 GRB 150911A gB 04 29 44.15 +05 44 07.6           ~ 29 0
13 GRB 121108A gB 05 32 46.58 +54 28 24.7           ~ 39 0
14 Fermi bn100619015 gB 05 38 28.0 -27 00 02           ~ 57 0
15 GRB 110801A gB 05 57 44.87 +80 57 21.1           ~ 90 0
16 GRB 200306A gB 06 44 24.65 -62 00 23.8           ~ 12 0
17 GRB 140430A gB 06 51 44.58 +23 01 25.5           ~ 81 0
18 GRB 061202 gB 07 02 06.190 -74 41 54.91           ~ 83 0
19 Fermi bn170208940 gB 08 30 -10.4           ~ 28 0
20 GRB 160117B gB 08 48 46.71 -16 22 00.9           ~ 41 0
21 GRB 050916 gB 09 03 57.270 -51 25 42.51           ~ 46 0
22 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
23 GRB 050502B gB 09 30 10.024 +16 59 48.07           ~ 169 0
24 Fermi bn140206304 gB 09 41 16.90 +66 45 42.7           ~ 149 0
25 GRB 111016A gB 10 15 20.16 +27 27 44.5           ~ 33 0
26 Fermi bn100727238 gB 10 16 42.67 -21 23 25.1           ~ 43 0
27 GRB 050714B gB 11 18 47.610 -15 32 48.90           ~ 80 0
28 GRB 110407A gB 12 24 07.47 +15 42 42.1           ~ 41 0
29 GRB 121229A gB 12 40 23.41 -50 35 37.2           ~ 57 0
30 GRB 160227A gB 12 59 13.71 +78 40 45.1           ~ 69 0
31 GRB 150222A gB 13 15 08.71 -12 09 07.5           ~ 28 0
32 GRB 090417B gB 13 58 44.8 +47 00 55           ~ 119 1
33 GRB 060204B gB 14 07 14.900 +27 40 36.40           ~ 93 0
34 Fermi bn170405777 gB 14 39 18.66 -25 14 36.9           ~ 75 0
35 GRB 141130A gB 14 51 17.28 +47 19 06.3           ~ 24 0
36 GRB 210724A gB 15 09 39.50 -06 17 27.3           ~ 13 0
37 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
38 GRB 051117A gB 15 13 34.020 +30 52 12.30 18.66 19.81       ~ 72 0
39 GRB 080212 gB 15 24 35.400 -22 44 29.50           ~ 58 0
40 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
41 Fermi bn151001628 gB 15 34 54.89 +10 58 01.9           ~ 19 0
42 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
43 GRB 060904A gB 15 50 54.560 +44 59 10.51           ~ 77 0
44 GRB 080210 gB 16 45 04.03 +13 49 36.3           ~ 121 0
45 GRB 060929 gB 17 32 28.920 +29 50 06.20           ~ 60 0
46 Fermi bn151027166 gB 18 09 56.87 +61 21 12.3           ~ 143 0
47 GRB 060111A gB 18 24 49.132 +37 36 14.47     18.86     ~ 72 0
48 Fermi bn120102095 gB 18 24 53.89 +24 42 47.1           ~ 42 0
49 GRB 180510A gB 18 25 19.69 -31 54 30.4           ~ 11 0
50 Fermi bn091026550 gB 18 26 -86.1           ~ 46 0
51 Fermi bn140506880 gB 18 27 06.04 -55 38 08.7           ~ 113 0
52 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
53 Fermi bn140713780 gB 18 44 25.13 +59 38 00.8           ~ 40 0
54 GRB 120514A gB 18 52 00.19 -04 15 48.9           ~ 40 0
55 Fermi bn100725475 gB 19 20 07 +76 57.3           ~ 55 0
56 GRB 210411C gB 19 46 26.74 -39 23 53.4           ~ 21 0
57 GRB 050607 gB 20 00 42.790 +09 08 31.50   19.55 18.94     ~ 103 0
58 GRB 050713A gB 21 22 09.530 +77 04 29.50           ~ 125 0
59 Fermi bn140108721 gB 21 40 26.77 +58 44 41.4           ~ 58 0
60 GRB 080506 gB 21 57 41.79 +38 59 06.7           ~ 46 0
61 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
62 Fermi bn081102739 gB 22 04 42.60 +52 59 27.7           ~ 60 0
63 GRB 110820A gB 22 52 46.10 +70 17 55.3           ~ 39 0

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