2026ApJ...998...62D


Query : 2026ApJ...998...62D

2026ApJ...998...62D - Astrophys. J., 998, 62 (2026/February-2)

Hierarchical Test of Lorentz Invariance with Gamma-Ray Burst Spectral-lag Measurements.

DU S.-S., GONG Y., WEI J.-J., LIU Z.-K., YOU Z.-Q., MENG Y.-Z. and ZHU X.-J.

Abstract (from CDS):

Gamma-ray bursts (GRBs) are among the most potent probes of Lorentz invariance violation (LIV), offering direct constraints on the quantum gravity energy scale (EQG) based on observations of energy-dependent time lags. Individual GRBs with well-defined positive-to-negative lag transitions have been used to set lower limits on EQG, but they suffer from uncertainties of spectral-lag measurements and systematics due to theoretical modeling of each burst. Here, we combine observations of 32 GRBs with positive-to-negative lag transitions to derive a statistically robust constraint on EQG through hierarchical Bayesian inference. We find that the dominant systematic uncertainty in LIV constraints arises from the intrinsic lag modeling. Accounting for this uncertainty with cubic spline interpolation, we derive robust limits of EQG,1 ≥ 4.37 × 1016 GeV for linear LIV and EQG,2 ≥ 3.02 × 108 GeV for quadratic LIV. We find that the probability for LIV, i.e., EQG,1 being below the Planck scale, is estimated to be around 90%, which we conclude as no significant evidence for LIV signatures in current GRB spectral lag observations. Our hierarchical approach provides a rigorous statistical framework for future LIV searches and can be extended to incorporate multimessenger observations.

Abstract Copyright: © 2026. The Author(s). Published by the American Astronomical Society.

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

Simbad objects: 32

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Number of rows : 32
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 bn150821406 gB 22 47 39.15 -57 53 38.2           ~ 71 0
31 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0
32 GRB 130518A gB 23 42 39.79 +47 27 55.2           ~ 86 0

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