2025MNRAS.543.2686F


Query : 2025MNRAS.543.2686F

2025MNRAS.543.2686F - Mon. Not. R. Astron. Soc., 543, 2686-2705 (2025/November-1)

Late-afterglow emission from a quasi-spherical outflow in a stratified environment.

FRAIJA N., BETANCOURT KAMENETSKAIA B., GALVAN A., MONTALVO A., DO ESPIRITO SANTO PEDREIRA A.C.C., VERES P., BECERRA R.L., DAINOTTI M.G., DICHIARA S. and VARGAS H.L.

Abstract (from CDS):

Gamma-ray bursts (GRBs) are cosmic events occurring at large distances beyond our galaxy. They provide a unique opportunity to study electromagnetic patterns not seen elsewhere. When the collimated GRB outflow interacts with the outer layers of a star or the wind generated by a binary neutron star merger, it releases energy, forming a quasi-spherical outflow around it. This broad outflow begins to radiate once it has transferred enough energy to the surrounding medium. We have developed a new analytical model that describes the synchrotron afterglow scenario of the quasi-spherical outflow, including factors such as stratified density, self-absorption regime, and the fraction of electrons accelerated by the shock front. We also successfully describe the multiwavelength observations of a sample of llGRB afterglows (GRB 980425, 031203, 060218, 100316D, 130603B, 150101B and 171205A) that exhibited a late component, analysed in both stellar wind and constant-density environments. Our analysis shows that a constant-density environment is favoured. Additionally, we consider the multiwavelength upper limits of the short bursts reported in the Swift-BAT data base.

Abstract Copyright: © The Author(s) 2025. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): acceleration of particles - radiation mechanisms: non-thermal - gamma-ray burst: individual: GRB 980425, 031203, 060218, 100316D, 130603B, 150101B and 171205A

Simbad objects: 22

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Number of rows : 22
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 070810B gB 00 35 48.4 +08 49 18           ~ 57 0
2 SN 2019oyw SN* 02 58 10.510 -08 57 27.20           ~ 218 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 050906 gB 03 31 15.28 -14 36 30.1           ~ 76 1
5 GRB 980923 gB 05 07.8 -80 36           ~ 51 0
6 SN 2010bh SN* 07 10 30.63 -56 15 19.7           SNIc 336 1
7 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 576 0
8 GRB 080121 gB 09 08 56.0 +41 50 29           ~ 40 0
9 1RXS J101702.9+353404 X 10 17 02.9 +35 34 04           ~ 4 0
10 Fermi bn100216422 gB 10 17 03 +35 31.0           ~ 32 0
11 SN 2009bb SN* 10 31 33.92 -39 57 28.2           SNIc 185 1
12 SN 2017iuk SN* 11 09 39.49 -12 35 18.7           SNII 210 0
13 LEDA 950703 EmG 11 09 39.661 -12 35 11.62   15.96   15.00   ~ 17 0
14 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
15 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
16 PS1-13arp SN* 12 18 25.108 +46 37 01.30           SNIIP 14 0
17 GALEX J123205.0-105600 Bz? 12 32 04.9717245480 -10 56 00.722548932         16.421 ~ 186 0
18 GRB 070810 gB 12 39.8 +10 45           ~ 16 0
19 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
20 SN 2020bvc SN* 14 33 57.009 +40 14 37.62           SNIc-BL 61 0
21 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
22 ESO 184-82 AG? 19 35 04.416 -52 50 38.04   15.17   14.26   ~ 113 2

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