2025A&A...695A.239B


Query : 2025A&A...695A.239B

2025A&A...695A.239B - Astronomy and Astrophysics, volume 695A239 (2025/3-1)

A comprehensive broadband analysis of the high-redshift GRB 240218A.

BRIVIO R., CAMPANA S., COVINO S., FERRO M., GIANFAGNA G., BERNARDINI M.G., D'AVANZO P., GIARRATANA S., GHIRLANDA G., HU Y.-D., MELANDRI A., NAVA L., PIRO L., ROSSI A., SALAFIA O.S., SALVAGGIO C., SALVATERRA R., SBARRATO T., SBARUFATTI B., TAGLIAFERRI G., THAKUR A.L., TOVMASSIAN G., AGUI FERNANDEZ J.F., BRUNI G., CASTRO-TIRADO A.J., D'ELIA V., DE PASQUALE M., DE UGARTE POSTIGO A., DE WET S., HARTMANN D.H., KLOSE S., KOBAYASHI S., MAIORANO E., MALESANI D.B., MARINI E., MARTIN-CARRILLO A., NICUESA GUELBENZU A., PANDEY S.B., PARIS D., PUGLIESE G., RAU A., RICCI R., SACCARDI A., SANCHEZ-RAMIREZ R., TANVIR N.R., THONE C.C. and ZAFAR T.

Abstract (from CDS):

Context. The detection and follow-up observations of high-redshift (z > 6) gamma-ray bursts (GRBs) provide a unique opportunity to explore the properties of the distant Universe. Unfortunately, they are rather rare, with only a dozen of them identified so far.
Aims. We present here the discovery of the GRB with the second highest spectroscopic redshift measured to date, GRB 240218A at z = 6.782, and the broadband analysis of its afterglow. Following the detection by high-energy satellites, we obtained multi-epoch and multi-wavelength photometric follow-up observations, from 68 s to ∼48 d after the detection. These data allow us to perform a comprehensive study of the emission and physical properties of this event. We also compare these properties with GRBs observed at high and low redshift.
Methods. We built the X-ray, near-infrared, and radio light curves and studied their temporal evolution. Moreover, we investigated the spectral energy distribution (SED) at different times to trace possible spectral evolution. We also compared the prompt phase properties, X-ray luminosity, and optical extinction of GRB 240218A with those of the long-duration GRB (LGRB) population.
Results. The SED analysis reveals a typical afterglow-like behaviour at late times. The origin of the early-time emission is uncertain, with the probable presence of an additional contribution on top of the afterglow emission. From the broadband physical modelling of the afterglow, we identify a narrow Gaussian jet seen slightly off-axis, $ \theta_{v}=2.52^{+0.57}_{-0.29}\,\mathrm{deg} $, and pinpoint the presence of a possible jet break ∼0.86 d after the trigger.
Conclusions. The results of the analysis and the comparison with other high-z GRBs reveal that we can consider GRB 240218A as a 'standard' high-redshift LGRB: the prompt phase properties, the X-ray luminosity, and the optical extinction are consistent with the values derived for the LGRB population. The jet opening angle is narrower but compatible with those of high-z bursts, possibly pointing to more collimated jets at high redshift.

Abstract Copyright: © The Authors 2025

Journal keyword(s): gamma-ray burst: general - gamma-ray burst: individual: GRB240218A

Simbad objects: 14

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Number of rows : 14
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 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
2 GRB 100905A gB 02 06 12.06 +14 55 45.9           ~ 45 0
3 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
4 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 213 0
5 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
6 GRB 240218A gB 10 47 11.24 +01 16 34.8           ~ 27 0
7 GRB 140515A gB 12 24 15.48 +15 06 17.7           ~ 90 0
8 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
9 GRB 090429B gB 14 02 40.10 +32 10 14.6           ~ 166 0
10 GRB 120521C gB 14 17 09.10 +42 08 39.8           ~ 93 0
11 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 185 0
12 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
13 GRB 120923A gB 20 15 10.73 +06 13 16.9           ~ 59 0
14 GRB 210905A gB 20 36 11.64 -44 26 24.3           ~ 42 0

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