2019ApJ...883..134T


Query : 2019ApJ...883..134T

2019ApJ...883..134T - Astrophys. J., 883, 134-134 (2019/October-1)

Closure relations of gamma-ray bursts in high energy emission.

TAK D., OMODEI N., UHM Z.L., RACUSIN J., ASANO K. and McENERY J.

Abstract (from CDS):

The synchrotron external shock model predicts the evolution of the spectral (β) and temporal (α) indices during the gamma-ray burst (GRB) afterglow for different environmental density profiles, electron spectral indices, electron cooling regimes, and regions of the spectrum. We study the relationship between α and β, the so-called "closure relations" with GRBs detected by Fermi Large Area Telescope (Fermi-LAT) from 2008 August to 2018 August. The spectral and temporal indices for the >100 MeV emission from the Fermi-LAT as determined in the Second Fermi-LAT Gamma-Ray Burst Catalog (2FLGC) are used in this work. We select GRBs whose spectral and temporal indices are well constrained (58 long-duration GRBs and 1 short-duration GRBs) and classify each GRB into the best-matched relation. As a result, we found that a number of GRBs require a very small fraction of the total energy density contained in the magnetic field (εB <= 10–7). The estimated mean and standard deviation of electron spectral index p are 2.40 and 0.44, respectively. The GRBs satisfying a closure relation of the slow cooling tend to have a softer p value compared to those of the fast cooling. Moreover, the Kolmogorov-Smirnov test of the two p distributions from the fast and slow coolings rejects a hypothesis that the two distributions are drawn from the single reference distribution with a significance of 3.2σ. Lastly, the uniform density medium is preferred over the medium that decreases like the inverse of distance squared for long-duration GRBs.

Abstract Copyright: © 2019. The American Astronomical Society. All rights reserved.

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

Simbad objects: 59

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Number of rows : 59
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 180720B gB 00 02 06.99 -02 55 07.8           ~ 215 0
2 Fermi bn180210517 gB 00 07 22.03 +18 33 09.6           ~ 15 0
3 Fermi bn110428388 gB 00 22 22.89 +64 50 56.8           ~ 26 0
4 Fermi bn180703876 gB 00 25 52.72 -67 10 47.9           ~ 35 0
5 Fermi bn131231198 gB 00 42 44.0 -01 29 40           ~ 103 0
6 Fermi bn160325291 gB 01 02 36.28 -72 41 48.5           ~ 52 0
7 Fermi bn120526303 gB 04 25 -32.2           ~ 15 0
8 GRB 171010A gB 04 26 19.41 -10 27 47.9           SNIc-BL 109 0
9 GRB 130502B gB 04 27 02.90 +71 03 38.5           ~ 31 0
10 Fermi bn091031500 gB 04 47 -57.5           ~ 33 0
11 GRB 090328 gB 06 02 39.69 -41 52 55.1           ~ 194 1
12 Fermi bn130504978 gB 06 06 31.29 +03 50 02.0           ~ 27 0
13 Fermi bn120711115 gB 06 18 42.839 -70 59 56.78           ~ 125 0
14 Fermi bn131014215 gB 06 41 12.80 -19 05 49.6           ~ 50 0
15 GRB 100511A gB 07 17.2 -04 39           ~ 28 0
16 GRB 150523A gB 07 41 08.67 -45 25 13.6           ~ 24 0
17 GRB 150627A gB 07 49 52.95 -51 29 22.5           ~ 24 0
18 Fermi bn140810782 gB 07 56 +27.5           ~ 19 0
19 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
20 Fermi bn130325203 gB 08 11 -18.9           ~ 13 0
21 GRB 140523A gB 08 52 26.70 +24 57 25.6           ~ 24 0
22 Fermi bn170808936 gB 09 43 +02.2           ~ 15 0
23 Fermi bn160521385 gB 09 50 39.92 +79 01 50.5           ~ 15 0
24 GRB 131108A gB 10 26 00.480 +09 39 44.05           ~ 96 0
25 GRB 141207A gB 10 40 +03.9           ~ 28 0
26 Fermi bn160905471 gB 10 48 59.06 -50 48 03.9           ~ 34 0
27 Fermi bn171120556 gB 10 55 09.80 +22 27 29.6           ~ 34 0
28 Fermi bn090626189 gB 11 20 -33.5           ~ 54 0
29 Fermi bn120624933 gB 11 23 31.98 +08 55 42.1           ~ 100 0
30 GRB 160821A gB 11 25 01 +42 20.7           ~ 71 0
31 GRB 120911B gB 11 28 35 -37 41.8           ~ 11 0
32 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
33 GRB 141222A gB 11 52 -57.4           ~ 16 0
34 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 244 1
35 Fermi bn100414097 gB 12 48 30.0 +08 41 35           ~ 136 0
36 Fermi bn131029973 gB 13 23 +48.3           ~ 13 0
37 Fermi bn170906030 gB 13 35 49.24 -47 06 03.4           ~ 33 0
38 Fermi bn150902733 gB 14 19 54.18 -69 21 09.9           ~ 30 0
39 GRB 130327B gB 14 31 30.57 -69 24 15.4           ~ 29 0
40 GRB 130606B gB 14 34 07.04 -22 06 08.2           ~ 47 0
41 Fermi bn170405777 gB 14 39 18.66 -25 14 36.9           ~ 75 0
42 Fermi bn081009140 gB 16 42 +18.4           ~ 40 0
43 GRB 091003A gB 16 46 04.680 +36 37 31.08           ~ 135 0
44 GRB 170214A gB 17 05 21.94 -01 53 14.9           ~ 54 0
45 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
46 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
47 GRB 110625A gB 19 06 55.85 +06 45 19.2           ~ 69 0
48 Fermi bn100116897 gB 20 20 +14.4           ~ 42 0
49 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 235 0
50 Fermi bn160509374 gB 20 47 00.90 +76 06 30.1           ~ 141 0
51 GRB 130821A gB 20 56 38.440 -12 02 36.53           ~ 25 0
52 GRB 160623A gB 21 01 11.54 +42 13 15.5           ~ 73 0
53 Fermi bn140206275 gB 21 01 -08.5           ~ 28 0
54 Fermi bn120709883 gB 21 14 -50.1           ~ 25 0
55 Fermi bn160816730 gB 21 29 38.70 +37 07 58.3           ~ 28 0
56 GRB 141028A gB 21 30 24.46 -00 13 55.6           ~ 109 0
57 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
58 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0
59 GRB 130518A gB 23 42 39.79 +47 27 55.2           ~ 86 0

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