2019MNRAS.485.2401W


Query : 2019MNRAS.485.2401W

2019MNRAS.485.2401W - Mon. Not. R. Astron. Soc., 485, 2401-2406 (2019/May-2)

New constraints on Lorentz invariance violation with polarized gamma-ray bursts.

WEI J.-J.

Abstract (from CDS):

Lorentz invariance violations (LIV) can yield vacuum birefringence, which results in an energy-dependent rotation of the polarization vector of linearly polarized emission from astrophysical sources. It is believed that if the relative rotation angle (ΔΘ) of the polarization vector of high-energy photons with respect to that of low-energy photons is larger than π/2, then the net polarization of the signal would be significantly depleted and could not be as high as the observed level. Hence, the measurement of high polarization implies that ΔΘ should not be too large. In this work, we assemble recent detections of prompt emission polarization in gamma-ray bursts (GRBs), all of whom have high detection significance. Following the method shown in Lin, Li & Chang (2016), we give a detailed calculation on the polarization evolution arising from the LIV effect for each GRB, and confirm that, even if ΔΘ is approaching to π/2, the net polarization is not severely suppressed, and more than 60 per cent of the initial polarization can be conserved. Applying this method to our GRB polarimetric data, we improve existing sensitivities to LIV involving photons by factors ranging from 2 to 10. In addition, we prove that our constraints are not greatly affected by uncertainties in the spectral parameters of GRBs.

Abstract Copyright: © 2019 The Author Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): astroparticle physics - gravitation - polarization - gamma-ray burst: general

Simbad objects: 21

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Number of rows : 21
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 041219 gB 00 24 27.7 +62 50 34           ~ 231 1
2 GRB 160607A gB 00 54 40.16 -04 56 54.5           ~ 22 0
3 Fermi bn160325291 gB 01 02 36.28 -72 41 48.5           ~ 52 0
4 GRB 160802A gB 02 21 +72.7           ~ 32 0
5 GRB 960924 gB 02 29.1 +02 42           ~ 30 0
6 GRB 160131A gB 05 12 40.31 -07 02 59.4           ~ 86 0
7 Fermi bn140206304 gB 09 41 16.90 +66 45 42.7           ~ 149 0
8 GRB 151006A gB 09 49 42.18 +70 30 10.5           ~ 42 0
9 GRB 160821A gB 11 25 01 +42 20.7           ~ 71 0
10 2B 930131 gB 12 08.2 -08 14           ~ 127 0
11 GRB 160910A gB 14 45 46.04 +39 04 01.3           ~ 45 0
12 GRB 110301A gB 15 17.4 +29 24           ~ 53 0
13 GRB 021206 gB 16 00 46.8 -09 42 36           ~ 112 0
14 GRB 100826A gB 18 56 -23.2           ~ 79 0
15 GRB 160703A gB 19 09 39 +36 54.8           ~ 33 0
16 GRB 061122A gB 20 15 19.840 +15 31 02.50           ~ 48 0
17 Fermi bn160509374 gB 20 47 00.90 +76 06 30.1           ~ 141 0
18 GRB 160623A gB 21 01 11.54 +42 13 15.5           ~ 73 0
19 GRB 110721A gB 22 10 -38.6           ~ 155 0
20 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
21 GRB 160106A gB ~ ~           ~ 10 0

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