2022ApJ...924L..29X


Query : 2022ApJ...924L..29X

2022ApJ...924L..29X - Astrophys. J., 924, L29-L29 (2022/January-2)

A robust estimation of Lorentz invariance violation and intrinsic spectral lag of short gamma-ray bursts.

XIAO S., XIONG S.-L., WANG Y., ZHANG S.-N., GAO H., ZHANG Z., CAI C., YI Q.-B., ZHAO Y., TUO Y.-L., LI X.-Q., WEN X.-Y., AN Z.-H., PENG W.-X., ZHENG S.-J., ZHANG F., SONG L.-M. and LI T.-P.

Abstract (from CDS):

Gamma-ray bursts (GRBs) have been identified as one of the most promising sources for Lorentz invariance violation (LIV) studies due to their cosmological distance and energetic emission in wide energy bands. However, the arrival-time difference of GRB photons among different energy bands is affected not only by the LIV effect but also by the poorly known intrinsic spectral lags. In previous studies, assumptions of spectral lag have to be made which could introduce systematic errors. In this paper, we used a sample of 46 short GRBs (SGRBs), whose intrinsic spectra lags are much smaller than long GRBs, to better constrain the LIV. The observed spectral lags are derived between two fixed energy bands in the source rest frame rather than the observer frame. Moreover, the lags are calculated with the novel Li-CCF method, which is more robust than traditional methods. Our results show that, if we consider LIV as a linear energy dependence of the photon propagation speed in the data fit, then we obtain a robust limit of EQG > 1015 GeV (95% CL). If we assume no LIV effect in the keV-MeV energy range, the goodness of data fit is equivalently as well as the case with LIV and we can constrain the common intrinsic spectral lags of SGRBs to be 1.4 ± 0.5 ms (1σ), which is the most accurate measurement thus far.

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

Journal keyword(s): Gamma-ray bursts

Simbad objects: 67

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Number of rows : 67
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 SDSS J002243.71-001657.5 G 00 22 43.71720 -00 16 57.5256           ~ 69 0
3 GRB 200826A gB 00 27 08.47 +34 01 36.5           ~ 121 0
4 Fermi bn150120123 G 00 41 16.5630 +33 59 42.598           ~ 70 0
5 Fermi bn100117879 G 00 45 04.6610 -01 35 42.020           ~ 155 0
6 Fermi bn111117510 gB 00 50 46.220 +23 00 39.22           ~ 141 0
7 GRB 181020A gB 00 55 55.77 -47 22 50.6           ~ 61 0
8 GRB 100625A gB 01 03 10.98 -39 05 18.3           ~ 124 0
9 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
10 PSO J047.1631+13.1580 G 03 08 39.14930640 +13 09 29.0253240           ~ 144 0
11 GRB 190114C gB 03 38 01.18 -26 56 47.8           ~ 343 0
12 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
13 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
14 GRB 060313 G 04 26 28.4020 -10 50 39.901 20.55 21.03 19.66     ~ 156 0
15 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
16 Fermi bn141004973 gB 05 06 56.11 +12 49 10.1           ~ 75 0
17 Fermi bn100728095 gB 05 55 02.00 -15 15 20.2           ~ 157 0
18 GRB 140213A gB 07 00 37.18 -73 08 14.1           ~ 102 0
19 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
20 Fermi bn150314205 gB 08 26 40.82 +63 50 03.4           ~ 117 0
21 SDSS J093805.33+153719.0 G 09 38 05.33384 +15 37 19.0406           ~ 146 0
22 Fermi bn111228657 gB 10 00 16.04 +18 17 52.2           ~ 201 0
23 GRB 160410A gB 10 02 44.37 +03 28 42.7           ~ 75 0
24 GRB 061217 gB 10 41 39.320 -21 07 22.11           ~ 128 0
25 GRB 201221D gB 11 24 14.19 +42 08 35.5           ~ 48 0
26 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
27 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
28 GRB 181123B G 12 17 27.9100 +14 35 52.270           ~ 47 0
29 GALEX J123205.0-105600 Bz? 12 32 04.9717245480 -10 56 00.722548932         16.421 ~ 186 0
30 SDSS J123612.87+285858.8 BiC 12 36 12.8803407000 +28 58 58.780075656           ~ 328 1
31 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
32 Fermi bn170705115 gB 12 49 +17.9           ~ 66 0
33 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 198 0
34 Fermi bn141220252 gB 13 00 15.70 +32 08 47.2           ~ 81 0
35 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
36 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
37 GRB 060801 G 14 12 01.2620 +16 58 55.970           ~ 172 0
38 GRB 150423A gB 14 46 18.96 +12 17 00.6           ~ 79 0
39 GRB 100628A gB 15 03 53.59 -31 39 50.4           ~ 50 0
40 GRB 120804A G 15 35 47.5100 -28 46 56.110           ~ 99 0
41 GRB 140903A G 15 52 03.2650 +27 36 10.710           ~ 138 0
42 GRB 190719C gB 16 00 49.50 +13 00 00.6           ~ 43 0
43 GRB 050813 gB 16 07 57.190 +11 14 57.80           ~ 147 0
44 GRB 190627A gB 16 19 18.73 -05 17 20.4           ~ 43 0
45 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
46 SN 2018fip SN* 16 54 15.64 -54 02 39.5           SNIc-BL 83 0
47 Fermi bn151027166 gB 18 09 56.87 +61 21 12.3           ~ 143 0
48 Fermi bn140506880 gB 18 27 06.04 -55 38 08.7           ~ 113 0
49 GRB 060502B gB 18 35 46.060 +52 37 51.45           ~ 153 1
50 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
51 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
52 Fermi bn140512814 gB 19 17 28.81 -15 05 39.5           ~ 133 0
53 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
54 Fermi bn131004904 gB 19 44 27.20 -02 57 31.0           ~ 113 0
55 Fermi bn121128212 gB 20 02 23.88 +54 17 59.1           ~ 128 0
56 GRB 210822A gB 20 17 44.99 +05 17 00.5           ~ 49 0
57 GRB 150403A gB 20 46 01.17 -62 42 40.1           ~ 116 0
58 GRB 140622A gB 21 08 41.56 -14 25 09.5           ~ 61 0
59 GRB 210619B gB 21 18 52.39 +33 51 00.2           ~ 93 0
60 GRB 070429B G 21 52 03.6910 -38 49 42.820           ~ 125 0
61 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
62 GRB 170428A G 22 00 18.7100 +26 54 56.280           ~ 52 0
63 GRB 051210 gB 22 00 40.930 -57 36 47.10           ~ 138 0
64 Fermi bn160624477 gB 22 00 46.21 +29 38 37.8           ~ 69 0
65 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
66 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
67 GRB 080123 gB 22 35 46.100 -64 54 03.24           ~ 98 0

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