2024A&A...690A.101W


Query : 2024A&A...690A.101W

2024A&A...690A.101W - Astronomy and Astrophysics, volume 690A101 (2024/10-1)

Investigating the off-axis GRB afterglow scenario for extragalactic fast X-ray transients.

WICHERN H.C.I., RAVASIO M.E., JONKER P.G., QUIROLA-VASQUEZ J.A., LEVAN A.J., BAUER F.E. and KANN D.A.

Abstract (from CDS):

Context. Extragalactic fast X-ray transients (FXTs) are short-duration (∼ks) X-ray flashes of unknown origin, potentially arising from binary neutron star (BNS) mergers, tidal disruption events, or supernova shock breakouts.
Aims. In the context of the BNS scenario, we investigate the possible link between FXTs and the afterglows of off-axis merger-induced gamma-ray bursts (GRBs).
Methods. By modelling well-sampled broadband afterglows of 13 merger-induced GRBs, we make predictions for their X-ray light curve behaviour had they been observed off-axis, considering both a uniform jet with core angle θC and a Gaussian-structured jet whose edge lies at an angle θW = 2θC. We compare their peak X-ray luminosity, duration, and temporal indices α (where F ∝ t^α^) with those of the currently known extragalactic FXTs.
Results. Our analysis reveals that a slightly off-axis observing angle of θobs ≈ (2.2 - 3)θC and a structured jet are required to explain the shallow (|α|≲0.3) temporal indices of the FXT light curves, which cannot be reproduced in the uniform-jet case at any viewing angle. In the case of a structured jet with truncation angle θW = 2θC, the distributions of the duration of the FXTs are consistent with those of the off-axis afterglows for the same range of observing angles, θobs ≈ (2.2 - 3)θC. While the distributions of the off-axis peak X-ray luminosity are consistent only for θobs = 2.2θC, focussing on individual events with different intrinsic luminosities reveals that the match of all three properties (peak X-ray luminosity, duration and temporal indices) of the FXTs at the same viewing angle is possible in the range θobs ∼ (2.2 - 2.6)θC. Despite the small sample of GRBs analysed, these results show that there is a region of the parameter space - although quite limited - where the observational properties of off-axis GRB afterglow can be consistent with those of the newly discovered FXTs. Future observations of FXTs discovered by the recently launched Einstein Probe mission and GRB population studies combined with more complex afterglow models will shed light on this possible GRB-FXT connection, and eventually unveil the progenitors of some FXTs.

Abstract Copyright: © The Authors 2024

Journal keyword(s): gamma-ray burst: general - X-rays: bursts - X-rays: general

Simbad objects: 38

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Number of rows : 38
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 Fermi bn111117510 gB 00 50 46.220 +23 00 39.22           ~ 141 0
2 CXO J010344.5-214845 X 01 03 44.59 -21 48 45.9           ~ 8 0
3 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
4 NAME XRT 161125 ? 02 26 51.57 -01 04 59.4           ~ 3 0
5 NAME XRT 151121 ? 02 43 19.13 +32 19 26.0           ~ 2 0
6 SN 2019oyw SN* 02 58 10.510 -08 57 27.20           ~ 218 0
7 NAME XRT 191223 ? 03 21 54.04 +41 14 49.3           ~ 3 0
8 NAME XRT 150322 ? 03 32 18.41 -27 52 24.4           ~ 7 0
9 NAME XRT 100831 ? 03 32 38.78 -27 51 33.8           ~ 5 0
10 [BTS2017] CDF-S XT1 G 03 32 38.8 -27 51 34           ~ 40 0
11 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
12 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
13 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
14 CXO J050706.7-315210 X 05 07 06.76 -31 52 10.8           ~ 9 0
15 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
16 GRB 051227 gB 08 20 58.107 +31 55 32.01           ~ 127 0
17 NAME GRB 060121 HOST Galaxy G 09 09 52.0260 +45 39 45.538       26.6   ~ 127 0
18 GRB 170807A gB 09 33 44 -17 20.9           ~ 8 0
19 GRB 160410A gB 10 02 44.37 +03 28 42.7           ~ 75 0
20 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
21 GRB 181123B G 12 17 27.9100 +14 35 52.270           ~ 47 0
22 NAME XRT 000519 X 12 25 31.64 +13 03 58.8           ~ 19 0
23 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
24 NAME XRT 210423 ev 13 48 56.46 +26 39 44.3           ~ 22 0
25 NAME XRT 191127 ? 13 49 23.31 +26 35 03.2           ~ 5 0
26 ACO 3581 ClG 14 07 29.8 -27 01 04           ~ 197 3
27 NAME XRT 110103 ev 14 08 28.89 -27 03 29.4           ~ 8 0
28 NAME XRT 140507 ? 15 34 56.39 +23 28 06.6           ~ 4 0
29 GRB 100702A gB 16 22 47.26 -56 31 53.8           ~ 53 0
30 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
31 GRB 071112B gB 17 20 51.0 -80 53 02           ~ 50 0
32 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
33 GRB 111020A gB 19 08 12.53 -38 00 43.0           ~ 66 0
34 GRB 110112A gB 21 59 43.77 +26 27 24.4           ~ 47 0
35 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
36 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
37 NVSS J230126-385839 rG 23 01 26.7650 -38 58 40.422   22.22 21.22 21   ~ 325 1
38 CXO J234503.4-423841 X 23 45 03.44 -42 38 41.7           ~ 11 0

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