2025A&A...703A..49B


Query : 2025A&A...703A..49B

2025A&A...703A..49B - Astronomy and Astrophysics, volume 703A49 (2025/11-1)

The most distant optically polarised GRB afterglow: GRB 240419A at z = 5.178.

BRIVIO R., COVINO S., FERRO M., SACCARDI A., MARTIN-CARRILLO A., KUWATA A., TOMA K., D'AVANZO P., HU Y.-D., IZZO L., KOBAYASHI S., LASKAR T., LELOUDAS G., MALESANI D.B., PURSIAINEN M., VERGANI S., WIERSEMA K., BLOEMEN S., CAMPANA S., D'ELIA V., DE WET S., DE PASQUALE M., GROOT P.J., JAKOBSSON P., MAO J., MELANDRI A., PUGLIESE G., ROSSI A., SALVATERRA R., SCHNEIDER B., TANVIR N.R., VAN ROESTEL J., VREESWIJK P.M. and ZAFAR T.

Abstract (from CDS):

Context. Gamma-ray bursts (GRBs) are extremely bright phenomena powered by relativistic jets arising from explosive events at cosmological distances. The nature of the jet and the configuration of the local magnetic fields are still unclear, with the distinction between different models possibly provided by the detection of early-time polarisation.
Aims. Past observations do not agree on a universal scenario describing early-time polarisation in GRB afterglows, and new studies are necessary to investigate this open question. We present here the discovery of GRB 240419A, its redshift determination of z = 5.178, its early-time optical polarimetry observations, and the multi-wavelength monitoring of its afterglow.
Methods. We analysed three epochs of polarimetric data to derive the early-time evolution of the polarisation. The multi-wavelength light curve from the X-rays to the near-infrared band was also investigated to give a broader perspective on the whole event.
Results. We find a high level of polarisation, $ P= 6.97^{+1.84}_{-1.52} $%, at 1740 s after the GRB trigger, followed by a slight decrease up to $ P= 4.81^{+1.87}_{-1.53} $% at 3059 s. On the same timescale, the polarisation position angle is nearly constant. The multi-band afterglow at the time of the polarisation measurements is consistent with a forward shock (FS), while the earlier evolution at t - t0 ≲ 700 s can be associated with the interplay between the forward and the reverse shocks or with energy injection.
Conclusions. The detected polarised radiation when the afterglow is FS-dominated and the stable position angle are consistent with an ordered magnetic field plus a turbulent component driven by large-scale magnetohydrodynamic instabilities. The lack of a jet break in the light curve prevents a comparison of the polarisation temporal evolution with theoretical expectations from magnetic fields amplified by microscopic-scale turbulence, limiting our ability to constrain the observer's viewing angle. Notably, GRB 240419A is the most distant GRB with a detected polarised optical afterglow, extending the redshift range for such measurements.

Abstract Copyright: © The Authors 2025

Journal keyword(s): polarization - gamma-ray burst: general - gamma-ray burst: individual: GRB 240419A

Simbad objects: 27

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Number of rows : 27
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 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
3 GRB 200826A gB 00 27 08.47 +34 01 36.5           ~ 121 0
4 CD-45 216B PM* 00 42 29.0676940152 -44 24 55.630436328   13.07 11.945 11.672   K4 17 1
5 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
6 Fermi bn091208410 gB 01 57 38.50 +16 52 50.7           ~ 220 0
7 GRB 191016A gB 02 01 04.67 +24 30 35.3           ~ 31 0
8 GRB 091018 gB 02 08 46 -57 33.0           ~ 169 0
9 GRB 190114C gB 03 38 01.18 -26 56 47.8           ~ 343 0
10 GRB 230307A gB 04 03 26.24 -75 22 43.8           ~ 221 0
11 GRB 121024A gB 04 41 53.31 -12 17 26.1           ~ 143 0
12 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
13 GRB 240419A gB 06 18 08.13 -44 59 57.6           ~ 2 0
14 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
15 CD-32 5613 WD* 08 41 32.4290850497 -32 56 32.915823461   12.07 11.85 12.3   DA5.5 325 0
16 GRB 191221B gB 10 19 19.17 -38 09 27.5           ~ 66 0
17 GRB 110205A gB 10 58 31.12 +67 31 31.2           ~ 213 0
18 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
19 SDSS J140910.47+275320.8 G 14 09 10.47535 +27 53 20.8393           ~ 279 0
20 GRB 120308A gB 14 36 20.02 +79 41 12.0           ~ 79 0
21 GRB 210610B gB 16 15 40.47 +14 23 56.3           ~ 87 0
22 CD-28 13479 * 17 43 19.5888438432 -28 40 32.665638756 11.17 11.36 10.61 10.46   B1II-III:nn 40 0
23 BD-12 5133 * 18 40 01.6961497488 -12 24 06.777653508 11.25 11.39 10.71 10.70   OB- 44 0
24 Fermi bn101112924 gB 19 28 54.9 +39 21 11           ~ 32 0
25 GRB 020813A gB 19 46 41.874 -19 36 04.81           ~ 316 0
26 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 235 0
27 GRB 210619B gB 21 18 52.39 +33 51 00.2           ~ 93 0

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