2023ApJ...949..110T


Query : 2023ApJ...949..110T

2023ApJ...949..110T - Astrophys. J., 949, 110 (2023/June-1)

Temporal and Spectral Evolution of Gamma-Ray Burst Broad Pulses: Identification of High-latitude Emission in the Prompt Emission.

TAK D., UHM Z.L., RACUSIN J., ZHANG B., GUIRIEC S., KOCEVSKI D., ZHANG B.-B. and McENERY J.

Abstract (from CDS):

We perform a detailed analysis of broad pulses in bright gamma-ray bursts (GRBs) to understand the evolution of GRB broad pulses. Using the temporal and spectral properties, we test the high-latitude emission (HLE) scenario in the decaying phase of broad pulses. The HLE originates from the curvature effect of a relativistic spherical jet, where higher-latitude photons are delayed and softer than the observer's line-of-sight emission. The signature of HLE has not yet been identified undisputedly during the prompt emission of GRBs. The HLE theory predicts a specific relation, ${F}_{\nu ,{E}_{p}}$ ∝ ${E}_{p}^{2}$, between the peak energy Ep in νFν spectra and the spectral flux Fν measured at Ep, ${F}_{\nu ,{E}_{p}}$. We search for evidence of this relation in 2157 GRBs detected by the Gamma-ray Burst Monitor on board the Fermi Gamma-ray Space Telescope from 2008 to 2017. After imposing unbiased selection criteria in order to minimize contamination in a signal by background and overlaps of pulses, we build a sample of 32 broad pulses in 32 GRBs. We perform a time-resolved spectral analysis on each of these 32 broad pulses and find that the evolution of 18 pulses (56%) is clearly consistent with the HLE relation. For the 18 broad pulses, the exponent δ in the relation of ${F}_{\nu ,{E}_{p}}$ ∝ Epδ is distributed as a Gaussian function with a median and width of 1.99 and 0.34, respectively. This result provides a constraint on the emission radius of GRBs with the HLE signature.

Abstract Copyright: © 2023. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Gamma-ray bursts - Relativistic jets

VizieR on-line data: <Available at CDS (J/ApJ/949/110): table1.dat table2.dat>

Simbad objects: 176

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Number of rows : 176
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 150306A gB 00 02 -58.5           ~ 9 0
2 Fermi bn161206064 gB 00 04 -34.0           ~ 4 0
3 Fermi bn131231198 gB 00 42 44.0 -01 29 40           ~ 103 0
4 Fermi bn150201574 gB 00 47 19.84 -37 37 07.8           ~ 30 0
5 Fermi bn081221681 gB 01 03 10.2 -24 32 53           ~ 186 0
6 GRB 150510A gB 01 05 +04.8           ~ 23 0
7 Fermi bn160118060 gB 01 10 52.8 +59 46 48           ~ 4 0
8 Fermi bn130425327 gB 01 11 -72.8           ~ 11 0
9 Fermi bn110921912 gB 01 12 -27.8           ~ 17 0
10 Fermi bn100322045 gB 01 25 -12.4           ~ 21 0
11 GRB 101014A gB 01 47.8 -51 04           ~ 31 0
12 Fermi bn140306146 gB 01 52 +49.0           ~ 12 0
13 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
14 GRB 120129A gB 02 02 +59.3           ~ 20 0
15 GRB 151107B gB 02 05 +45.6           ~ 13 0
16 GRB 160802A gB 02 21 +72.7           ~ 32 0
17 GRB 140416A gB 02 22 +43.9           ~ 17 0
18 Fermi bn100324172 gB 02 39 -19.3           ~ 21 0
19 Fermi bn160422499 gB 02 45 -58.2           ~ 6 0
20 Fermi bn091030828 gB 02 47 +21.5           ~ 17 0
21 Fermi bn100701490 gB 02 52 -02.2           ~ 20 0
22 Fermi bn121122885 gB 02 56 +48.2           ~ 9 0
23 GRB 110825A gB 02 59.6 +15 24           ~ 33 0
24 Fermi bn160421137 gB 03 09 +62.8           ~ 3 0
25 Fermi bn130609902 gB 03 35 05.11 -40 10 26.7           ~ 54 0
26 Fermi bn120316008 gB 03 48 -56.3           ~ 17 0
27 GRB 131028A gB 03 48 +72.2           ~ 14 0
28 GRB 160720A gB 03 52 36.7 +73 53 35           ~ 12 0
29 Fermi bn151231443 gB 04 22 -61.5           ~ 7 0
30 Fermi bn130704560 gB 04 22 -14.5           ~ 5 0
31 Fermi bn161020759 gB 04 24 -75.7           ~ 4 0
32 Fermi bn120526303 gB 04 25 -32.2           ~ 15 0
33 GRB 171010A gB 04 26 19.41 -10 27 47.9           SNIc-BL 109 0
34 GRB 130502B gB 04 27 02.90 +71 03 38.5           ~ 31 0
35 GRB 170121B gB 04 51 -12.7           ~ 9 0
36 Fermi bn161229878 gB 05 24 +06.3           ~ 10 0
37 GRB 131229A gB 05 40 55.61 -04 23 46.6           ~ 35 0
38 Fermi bn150202999 gB 05 47 49.07 +58 49 46.7           ~ 14 0
39 GRB 090820 gB 05 51 +27.1           ~ 44 0
40 Fermi bn100728095 gB 05 55 02.00 -15 15 20.2           ~ 157 0
41 GRB 090328 gB 06 02 39.69 -41 52 55.1           ~ 194 1
42 Fermi bn130504978 gB 06 06 31.29 +03 50 02.0           ~ 27 0
43 GRB 090717A gB 06 10 -62.5           ~ 33 0
44 Fermi bn120711115 gB 06 18 42.839 -70 59 56.78           ~ 125 0
45 GRB 150213A gB 06 21 -04.8           ~ 15 0
46 Fermi bn110407998 gB 06 30 -11.9           ~ 10 0
47 Fermi bn141222691 gB 06 30 +40.1           ~ 4 0
48 GRB 130304A gB 06 36 +53.6           ~ 4 0
49 Fermi bn131014215 gB 06 41 12.80 -19 05 49.6           ~ 50 0
50 Fermi bn141029134 gB 06 50 +25.1           ~ 8 0
51 Fermi bn120728434 gB 06 55 -45.9           ~ 12 0
52 GRB 080723D gB 07 01 +71.1           ~ 18 0
53 GRB 100511A gB 07 17.2 -04 39           ~ 28 0
54 GRB 150210A gB 07 28.6 +13 16           ~ 21 0
55 GRB 100719D gB 07 33 +05.4           ~ 20 0
56 GRB 150523A gB 07 41 08.67 -45 25 13.6           ~ 24 0
57 Fermi bn130305486 gB 07 46 59.45 +52 02 00.2           ~ 35 0
58 GRB 150627A gB 07 49 52.95 -51 29 22.5           ~ 24 0
59 Fermi bn140810782 gB 07 56 +27.5           ~ 19 0
60 Fermi bn141022087 gB 07 58 -75.2           ~ 5 0
61 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
62 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 193 0
63 GRB 081215A gB 08 22 +54.0           ~ 57 0
64 Fermi bn150314205 gB 08 26 40.82 +63 50 03.4           ~ 117 0
65 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
66 GRB 101123A gB 08 45.0 +06 31           ~ 27 0
67 Fermi bn170921168 gB 08 49 30.0 +57 03 25           ~ 9 0
68 GRB 140523A gB 08 52 26.70 +24 57 25.6           ~ 24 0
69 GRB 160530B gB 08 54 +43.5           ~ 14 0
70 Fermi bn110622158 gB 08 56 +19.5           ~ 12 0
71 GRB 171119A gB 09 02 -47.0           ~ 10 0
72 Fermi bn150220598 gB 09 02 -01.6           ~ 13 0
73 Fermi bn140329295 gB 09 43 -32.2           ~ 17 0
74 Fermi bn170808936 gB 09 43 +02.2           ~ 15 0
75 GRB 080817 gB 10 05 09.600 -19 15 36.00           ~ 27 0
76 GRB 131108A gB 10 26 00.480 +09 39 44.05           ~ 96 0
77 GRB 141207A gB 10 40 +03.9           ~ 28 0
78 Fermi bn170510217 gB 10 40 36.94 -39 12 45.0           ~ 21 0
79 Fermi bn160905471 gB 10 48 59.06 -50 48 03.9           ~ 34 0
80 Fermi bn090626189 gB 11 20 -33.5           ~ 54 0
81 Fermi bn120624933 gB 11 23 31.98 +08 55 42.1           ~ 100 0
82 GRB 160821A gB 11 25 01 +42 20.7           ~ 71 0
83 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
84 GRB 140821A gB 11 39 +13.5           ~ 6 0
85 Fermi bn140721336 gB 11 43 -41.2           ~ 3 0
86 GRB 080723B gB 11 47 19.77 -60 14 27.9           ~ 53 0
87 Fermi bn141215560 gB 11 56 -52.7           ~ 3 0
88 Fermi bn160106948 gB 12 06 +17.5           ~ 2 0
89 GRB 131214A gB 12 16 -06.3           ~ 4 0
90 Fermi bn160113398 gB 12 29 02.4 +11 31 48           ~ 15 0
91 Fermi bn171102107 gB 12 31 +54.0           ~ 13 0
92 GRB 170115B gB 12 36 -46.9           ~ 25 0
93 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
94 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 244 1
95 Fermi bn100414097 gB 12 48 30.0 +08 41 35           ~ 136 0
96 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 198 0
97 Fermi bn170527480 gB 13 01 +00.9           ~ 16 0
98 GRB 081224A gB 13 26.8 +75 06           ~ 32 0
99 Fermi bn170906030 gB 13 35 49.24 -47 06 03.4           ~ 33 0
100 Fermi bn090217206 gB 13 40 -08.4           ~ 56 0
101 Fermi bn110920338 gB 13 59 -27.6           ~ 28 0
102 Fermi bn130121835 gB 14 05 -49.5           ~ 5 0
103 Fermi bn150902733 gB 14 19 54.18 -69 21 09.9           ~ 30 0
104 GRB 130327B gB 14 31 30.57 -69 24 15.4           ~ 29 0
105 GRB 130606B gB 14 34 07.04 -22 06 08.2           ~ 47 0
106 Fermi bn170405777 gB 14 39 18.66 -25 14 36.9           ~ 75 0
107 Fermi bn170614486 gB 14 43 +47.5           ~ 4 0
108 GRB 160910A gB 14 45 46.04 +39 04 01.3           ~ 45 0
109 Fermi bn170210116 gB 15 04 -65.1           ~ 16 0
110 GRB 120328B gB 15 12 +22.8           ~ 24 0
111 GRB 110301A gB 15 17.4 +29 24           ~ 53 0
112 GRB 080825C gB 15 28.8 -04 54           ~ 71 0
113 Fermi bn110709642 gB 15 55 33.95 +40 55 27.4       21.4   ~ 59 0
114 Fermi bn170228794 gB 15 58 -03.6           ~ 13 0
115 Fermi bn150118409 gB 16 01 -35.8           ~ 18 0
116 Fermi bn110102788 gB 16 23 31.41 +07 36 49.8           ~ 62 0
117 GRB 170607B gB 16 27 -39.2           ~ 10 0
118 Fermi bn110123804 gB 16 28 +28.0           ~ 13 0
119 Fermi bn081009140 gB 16 42 +18.4           ~ 40 0
120 GRB 091003A gB 16 46 04.680 +36 37 31.08           ~ 135 0
121 GRB 150213B gB 16 53 48.56 +34 11 19.6           ~ 27 0
122 GRB 140508A gB 17 01 51.95 +46 46 49.5           ~ 76 0
123 GRB 170214A gB 17 05 21.94 -01 53 14.9           ~ 54 0
124 GRB 131122B gB 17 27 +33.4           ~ 4 0
125 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
126 Fermi bn111220486 gB 17 50 -56.0           ~ 12 0
127 Fermi bn150309958 gB 18 28 24.81 +86 25 43.6           ~ 30 0
128 GRB 130306A gB 18 37 50.75 -11 40 52.4           ~ 28 0
129 Fermi bn110919634 gB 18 40 +66.4           ~ 10 0
130 GRB 171227A gB 18 43 -35.0           ~ 27 0
131 GRB 100826A gB 18 56 -23.2           ~ 79 0
132 GRB 110625A gB 19 06 55.85 +06 45 19.2           ~ 69 0
133 Fermi bn130715906 gB 19 10 -31.1           ~ 6 0
134 Fermi bn151227218 gB 19 12 +31.9           ~ 5 0
135 Fermi bn140512814 gB 19 17 28.81 -15 05 39.5           ~ 133 0
136 GRB 120707A gB 19 24 -34.4           ~ 21 0
137 Fermi bn120204054 gB 19 30 -03.6           ~ 11 0
138 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
139 Fermi bn151030999 gB 19 50 31.2 +30 51 00           ~ 6 0
140 Fermi bn160107931 gB 19 58 40.8 +06 24 47           ~ 12 0
141 Fermi bn170511249 gB 20 02 +33.3           ~ 6 0
142 GRB 120226A gB 20 12 +48.7           ~ 22 0
143 Fermi bn130219775 gB 20 15 +40.8           ~ 9 0
144 Fermi bn100116897 gB 20 20 +14.4           ~ 42 0
145 Fermi bn131127592 gB 20 24 -00.8           ~ 17 0
146 GRB 100918A gB 20 34 -46.0           ~ 15 0
147 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 235 0
148 Fermi bn121225417 gB 20 42 -34.8           ~ 13 0
149 GRB 100528A gB 20 44 29 +27 48.6           ~ 37 0
150 GRB 150403A gB 20 46 01.17 -62 42 40.1           ~ 116 0
151 Fermi bn160509374 gB 20 47 00.90 +76 06 30.1           ~ 141 0
152 GRB 090528B gB 20 49 +32.7           ~ 30 0
153 Fermi bn110717319 gB 20 51 -14.8           ~ 15 0
154 GRB 130821A gB 20 56 38.440 -12 02 36.53           ~ 25 0
155 Fermi bn140206275 gB 21 01 -08.5           ~ 28 0
156 Fermi bn170207906 gB 21 03 +55.7           ~ 15 0
157 GRB 101023A gB 21 11 51.26 -65 23 17.7           ~ 71 0
158 Fermi bn160816730 gB 21 29 38.70 +37 07 58.3           ~ 28 0
159 GRB 141028A gB 21 30 24.46 -00 13 55.6           ~ 109 0
160 Fermi bn170826819 gB 21 50 48.0 -31 48 00           ~ 9 0
161 Fermi bn090829672 gB 21 56.8 -34 12           ~ 30 0
162 Fermi bn150330828 gB 21 57 +50.0           ~ 22 0
163 GRB 110721A gB 22 10 -38.6           ~ 155 0
164 Fermi bn171210493 gB 22 21 09.6 +24 26 24           ~ 20 0
165 Fermi bn130720582 gB 22 32 -09.4           ~ 8 0
166 GRB 090719 gB 22 45 -67.9           ~ 41 0
167 Fermi bn150821406 gB 22 47 39.15 -57 53 38.2           ~ 71 0
168 Fermi bn170409112 gB 23 10 -07.1           ~ 18 0
169 GRB 131118A gB 23 20 -66.8           ~ 10 0
170 GRB 150724B gB 23 27 33.88 +03 49 06.4           ~ 17 0
171 GRB 110729A gB 23 34 +05.0           ~ 15 0
172 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0
173 GRB 130518A gB 23 42 39.79 +47 27 55.2           ~ 86 0
174 Fermi bn160215773 gB 23 47 09.6 +01 43 48           ~ 10 0
175 Fermi bn140323433 gB 23 47 50.31 -79 54 16.4           ~ 36 0
176 Fermi bn161218356 gB 23 54 -16.9           ~ 21 0

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