2017ApJ...837..119A

Query : 2017ApJ...837..119A

2017ApJ...837..119A - Astrophys. J., 837, 119-119 (2017/March-2)

The maximum isotropic energy of gamma-ray bursts.

ATTEIA J.-L., HEUSSAFF V., DEZALAY J.-P., KLOTZ A., TURPIN D., TSVETKOVA A.E., FREDERIKS D.D., ZOLNIEROWSKI Y., DAIGNE F. and MOCHKOVITCH R.

Abstract (from CDS):

The most energetic gamma-ray bursts (GRBs) are remarkable sources releasing huge amounts of energy on short timescales. Their prompt emission, which usually lasts a few seconds, is so bright that it is visible across the whole observable universe. Studying these extreme events may provide clues on the nature of GRB progenitors and on the physical processes at work in relativistic jets. In this paper, we study the bright end of the isotropic energy distribution of long GRBs. We use two samples of long GRBs with redshift detected by Fermi/GBM or Konus-Wind, two instruments that measure the spectral shape and the energetics of the prompt emission accurately. We focus on GRBs within a range of redshifts z = 1-5, a volume that contains a large number of energetic GRBs, and we propose a simple method to reconstruct the bright end of the GRB energy distribution from the observed one. We find that the GRB energy distribution cannot be described by a simple power law but requires a strong cutoff above 1–3×1054 erg. We attribute this feature to an intrinsic limit on the energy per unit of solid angle radiated by GRBs.

Abstract Copyright: © 2017. The American Astronomical Society. All rights reserved.

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

Errata: erratum vol. 852, art. 144 (2018)

Simbad objects: 101

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Number of rows : 101
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 bn160629930 gB 00 19 27.17 +76 58 02.4           ~ 39 0
2 GRB 150206A gB 00 40 17.57 -63 10 56.0           ~ 55 0
3 Fermi bn140703026 gB 00 51 58.99 +45 06 05.4           ~ 90 0
4 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
5 Fermi bn081221681 gB 01 03 10.2 -24 32 53           ~ 186 0
6 Fermi bn100814160 gB 01 29 53.61 -17 59 43.6           ~ 219 0
7 GRB 081222 gB 01 30 57.76 -34 05 44.0           ~ 199 0
8 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
9 Fermi bn091208410 gB 01 57 38.50 +16 52 50.7           ~ 220 0
10 Fermi bn090113778 gB 02 08 16.00 +33 26 08.4           ~ 92 0
11 GRB 131011A gB 02 10 06.11 -04 24 42.5           ~ 45 0
12 GRB 110918A gB 02 10 09.39 -27 06 19.6           ~ 83 0
13 GRB 000911 gB 02 18 42 +07 48.0           ~ 163 0
14 GRB 080411 gB 02 31 54.82 -71 18 07.5           ~ 109 0
15 GRB 050603 gB 02 39 56.839 -25 10 54.92     18.48     ~ 174 0
16 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
17 Fermi bn100728439 gB 02 56 13.44 +00 16 51.6           ~ 142 0
18 GRB 140801A gB 02 56 16.50 +30 56 16.8           ~ 55 0
19 Fermi bn090926914 gB 03 05 14.30 -38 59 50.9           ~ 149 1
20 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 315 1
21 GRB 140907A gB 03 12 34.98 +46 36 17.2           ~ 81 0
22 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 127 0
23 GRB 070328 gB 04 20 27.680 -34 04 00.60 20.29         ~ 97 0
24 Fermi bn131105087 gB 04 43 53.50 -63 00 17.7           ~ 95 0
25 GRB 060124 gB 05 08 25.900 +69 44 26.98   18.91 17.35     ~ 280 0
26 GRB 991216 gB 05 09 31.2983 +11 17 07.262           ~ 430 0
27 Fermi bn100728095 gB 05 55 02.00 -15 15 20.2           ~ 157 0
28 GRB 081121 gB 05 57 07.70 -60 36 42.1           ~ 152 0
29 GRB 090201 gB 06 08 12.30 -46 36 16.1           ~ 68 0
30 GRB 000131 gB 06 13 31.08 -51 56 41.7     24.7     ~ 172 1
31 Fermi bn120711115 gB 06 18 42.839 -70 59 56.78           ~ 125 0
32 GRB 140213A gB 07 00 37.18 -73 08 14.1           ~ 102 0
33 GRB 110422A gB 07 28 11.21 +75 06 24.0           ~ 113 0
34 GRB 070125 gB 07 51 17.80 +31 09 04.8           ~ 188 0
35 GRB 071020 gB 07 58 39.65 +32 51 38.8           ~ 158 0
36 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
37 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 193 0
38 Fermi bn150314205 gB 08 26 40.82 +63 50 03.4           ~ 117 0
39 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
40 GRB 110503A gB 08 51 06.31 +52 12 27.7           ~ 115 0
41 GRB 130408A gB 08 57 37.30 -32 21 38.9           ~ 98 0
42 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
43 GRB 130505A gB 09 17 21.9014988888 +01 42 03.426207768           ~ 94 0
44 Fermi bn140206304 gB 09 41 16.90 +66 45 42.7           ~ 149 0
45 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
46 GRB 131108A gB 10 26 00.480 +09 39 44.05           ~ 96 0
47 Fermi bn120624933 gB 11 23 31.98 +08 55 42.1           ~ 100 0
48 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
49 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
50 GRB 080603B gB 11 46 07.46 +68 03 38.5           ~ 153 0
51 GRB 160625A gB 11 47 39.82 -65 08 41.1           ~ 25 0
52 Fermi bn100615083 gB 11 48 49.25 -19 28 52.2           ~ 133 0
53 GRB 990506 gB 11 54 41 -26 45.0           ~ 169 1
54 GRB 000418 gB 12 25 21 +20 05.0           ~ 219 0
55 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 244 1
56 Fermi bn100414097 gB 12 48 30.0 +08 41 35           ~ 136 0
57 GRB 080607A gB 12 59 47.14 +15 55 09.6           ~ 257 0
58 Fermi bn141220252 gB 13 00 15.70 +32 08 47.2           ~ 81 0
59 Fermi bn140423356 gB 13 09 06.20 +49 50 18.3           ~ 114 0
60 Fermi bn141221338 gB 13 13 09.02 +08 12 18.3           ~ 76 0
61 GRB 051008 gB 13 31 28.100 +42 08 05.01 17.06   14.11     ~ 90 0
62 GRB 990510 gB 13 38 07.64 -80 29 48.8           ~ 499 1
63 GRB 130907A gB 14 23 34.03 +45 36 27.1           ~ 120 0
64 Fermi bn140808038 gB 14 44 53.27 +49 12 52.7           ~ 45 0
65 GRB 010222 G 14 52 12.5 +43 01 06           ~ 364 1
66 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 180 0
67 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 1012 1
68 GRB 070521 gB 16 10 38.600 +30 15 22.70           ~ 164 0
69 Fermi bn150301045 gB 16 17 13.13 -48 42 47.2           ~ 31 0
70 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
71 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 185 0
72 GRB 140508A gB 17 01 51.95 +46 46 49.5           ~ 76 0
73 GRB 000926 gB 17 04 15 +51 46.0           ~ 373 0
74 GRB 120811A gB 17 08 44.10 -22 44 06.7           ~ 16 0
75 GRB 080319C gB 17 15 55.48 +55 23 31.7           ~ 174 0
76 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
77 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
78 Fermi bn120326056 gB 18 15 37.06 +69 15 35.4           ~ 188 0
79 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
80 Fermi bn140620219 gB 18 47 29.00 +49 43 51.0           ~ 37 0
81 GRB 090709A gB 19 19 46.70 +60 43 40.8           ~ 125 0
82 GRB 020813A gB 19 46 41.874 -19 36 04.81           ~ 316 0
83 Fermi bn121128212 gB 20 02 23.88 +54 17 59.1           ~ 128 0
84 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 181 0
85 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 235 0
86 GRB 150403A gB 20 46 01.17 -62 42 40.1           ~ 116 0
87 Fermi bn160509374 gB 20 47 00.90 +76 06 30.1           ~ 141 0
88 Fermi bn120716712 gB 20 52 12.17 +09 35 53.9           ~ 72 0
89 GRB 141028A gB 21 30 24.46 -00 13 55.6           ~ 109 0
90 GRB 080514B gB 21 31 22.61 +00 42 30.3           ~ 69 0
91 Fermi bn080804972 gB 21 54 41.90 -53 11 20.2           ~ 158 0
92 GRB 071117 gB 22 20 10.40 -63 26 36.6           ~ 112 0
93 GRB 151021A gB 22 30 34.43 -33 11 50.4           ~ 72 0
94 Fermi bn091024380 gB 22 37 +56.9           ~ 151 0
95 GRB 131030A gB 23 00 16.14 -05 22 05.2           ~ 126 0
96 GRB 100606A gB 23 22 30.49 -66 14 28.6           ~ 46 0
97 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0
98 GRB 130518A gB 23 42 39.79 +47 27 55.2           ~ 86 0
99 Fermi bn080810549 gB 23 47 08.00 +00 18 35.1           ~ 240 0
100 GRB 130701A gB 23 48 55.05 +36 06 01.2           ~ 81 0
101 GRB 061222A gB 23 53 03.419 +46 31 58.60           ~ 177 0

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