2022ApJ...935...79L


Query : 2022ApJ...935...79L

2022ApJ...935...79L - Astrophys. J., 935, 79 (2022/August-3)

Spectral Lag Transition of 32 Fermi Gamma-Ray Bursts and Their Application on Constraining Lorentz Invariance Violation.

LIU Z.-K., ZHANG B.-B. and MENG Y.-Z.

Abstract (from CDS):

The positive-to-negative transition of spectral lag is an uncommon feature reported in a small number of gamma-ray bursts (GRBs). An application of such a feature has been made to constrain the critical quantum gravity energy (EQG) of the light photons under the hypothesis that the Lorentz invariance might be violated. Motivated by previous case studies, this paper systematically examined the up-to-date GRB sample observed by Fermi Gamma-ray Burst Monitor for the lag transition feature to establish a comprehensive physical limit on the Lorentz invariance violation (LIV). This search resulted in 32 GRBs with redshift available, which exhibit the lag transition phenomenon. We first fit each of the lag-E relations of the 32 GRBs with an empirical smoothly broken power-law function, and found that the lag transition occurs typically at about 400 keV. We then implemented the LIV effect into the fit, which enabled us to constrain the lower limit of the linear and quadratic values of EQG, which are typically distributed at 1.5 × 1014 and 8 × 105 GeV, respectively.

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

Journal keyword(s): Gamma-ray bursts - Gravitation - Quantum gravity

Simbad objects: 33

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Number of rows : 33
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 bn180703876 gB 00 25 52.72 -67 10 47.9           ~ 35 0
3 Fermi bn131231198 gB 00 42 44.0 -01 29 40           ~ 103 0
4 Fermi bn081221681 gB 01 03 10.2 -24 32 53           ~ 186 0
5 GRB 201216C gB 01 05 28.88 +16 30 58.0           ~ 89 0
6 Fermi bn130925164 gB 02 44 42.38 -26 09 15.8           ~ 184 0
7 GRB 190114C gB 03 38 01.18 -26 56 47.8           ~ 343 0
8 GRB 171010A gB 04 26 19.41 -10 27 47.9           SNIc-BL 109 0
9 Fermi bn150514774 gB 04 59 30.45 -60 58 07.0           ~ 51 0
10 Fermi bn100728095 gB 05 55 02.00 -15 15 20.2           ~ 157 0
11 GRB 090328 gB 06 02 39.69 -41 52 55.1           ~ 194 1
12 GRB 210204A gB 07 48 19.37 +11 24 34.2           ~ 46 0
13 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
14 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 193 0
15 Fermi bn150314205 gB 08 26 40.82 +63 50 03.4           ~ 117 0
16 Fermi bn140206304 gB 09 41 16.90 +66 45 42.7           ~ 149 0
17 GRB 200613A gB 10 12 10.03 +45 45 14.1           ~ 36 0
18 GRB 131108A gB 10 26 00.480 +09 39 44.05           ~ 96 0
19 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
20 GRB 210610B gB 16 15 40.47 +14 23 56.3           ~ 87 0
21 GRB 200829A gB 16 44 49.42 +72 19 45.3           ~ 55 0
22 GRB 091003A gB 16 46 04.680 +36 37 31.08           ~ 135 0
23 GRB 140508A gB 17 01 51.95 +46 46 49.5           ~ 76 0
24 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
25 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 235 0
26 GRB 150403A gB 20 46 01.17 -62 42 40.1           ~ 116 0
27 Fermi bn160509374 gB 20 47 00.90 +76 06 30.1           ~ 141 0
28 GRB 210619B gB 21 18 52.39 +33 51 00.2           ~ 93 0
29 GRB 141028A gB 21 30 24.46 -00 13 55.6           ~ 109 0
30 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
31 Fermi bn150821406 gB 22 47 39.15 -57 53 38.2           ~ 71 0
32 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0
33 GRB 130518A gB 23 42 39.79 +47 27 55.2           ~ 86 0

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