2024MNRAS.533.1629O


Query : 2024MNRAS.533.1629O

2024MNRAS.533.1629O - Mon. Not. R. Astron. Soc., 533, 1629-1648 (2024/September-2)

X-ray afterglow limits on the viewing angles of short gamma-ray bursts.

O'CONNOR B., BENIAMINI P. and GILL R.

Abstract (from CDS):

The behaviour of a short gamma-ray burst (sGRB) afterglow light curve can reveal the angular structure of the relativistic jet and constrain the observer's viewing angle $\theta _\textrm {obs}$. The observed deceleration time of the jet, and, therefore, the time of the afterglow peak, depends on the observer's viewing angle. A larger viewing angle leads to a later peak of the afterglow and a lower flux at peak. We utilize the earliest afterglow detections of 58 sGRBs detected with the Neil Gehrels Swift Observatory X-ray Telescope to constrain the ratio of the viewing angle $\theta _\textrm {obs}$ to the jet's core $\theta _\textrm {c}$. We adopt a power-law angular jet structure in both energy $E(\theta)\propto \theta ^{-a}$ and Lorentz factor $\Gamma (\theta)\propto \theta ^{-b}$ beyond the core. We find that either sGRBs are viewed within $\theta _\textrm {obs}/\theta _\textrm {c}\lt 1$ or the initial Lorentz factor of material in their jet's core is extremely high ($\Gamma _0\gt 500$). If we consider tophat jets, we constrain 90 per cent of our sample to be viewed within $\theta _\textrm {obs}/\theta _\textrm {c}\lt 1.06$ and 1.15 for our canonical and conservative afterglow scenarios. For a subset of events with measurements of the jet break, we can constrain $\Gamma _0\theta _\textrm {c}\gtrsim 30$. This confirmation that cosmological sGRBs are viewed either on-axis or very close to their jet's core has significant implications for the nature of the prompt gamma-ray production mechanism and for the rate of future sGRB detections coincident with gravitational waves, implying that they are extremely rare.

Abstract Copyright: © 2024 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): stars: jets - gamma-ray bursts - neutron star mergers

Simbad objects: 63

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Number of rows : 63
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 SDSS J002243.71-001657.5 G 00 22 43.71720 -00 16 57.5256           ~ 69 0
2 GRB 140930B gB 00 25 23.40 +24 17 41.7           ~ 52 0
3 Fermi bn111117510 gB 00 50 46.220 +23 00 39.22           ~ 141 0
4 GRB 100625A gB 01 03 10.98 -39 05 18.3           ~ 124 0
5 GRB 230228A gB 01 13 30.74 +44 28 58.5           ~ 20 0
6 GRB 151127A gB 01 17 54.58 -82 46 15.0           ~ 18 0
7 Fermi bn170127634 gB 01 19 54.47 -30 21 28.6           ~ 36 0
8 GRB 080426 gB 01 45 59.79 +69 28 06.0           ~ 50 0
9 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
10 Fermi bn081024245 gB 01 51 33.80 +61 21 08.2           ~ 75 0
11 GRB 141212A G 02 36 29.9570 +18 08 47.228           ~ 70 0
12 GRB 120305A gB 03 10 08.73 +28 29 30.9           ~ 56 0
13 Fermi bn130912358 gB 03 10 25.60 +13 59 55.7           ~ 57 0
14 GRB 200411A gB 03 10 39.39 -52 19 03.3           ~ 31 0
15 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
16 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
17 GRB 230307A gB 04 03 26.24 -75 22 43.8           ~ 221 0
18 GRB 201006A gB 04 07 34.25 +65 09 52.8           ~ 30 0
19 GRB 060313 G 04 26 28.4020 -10 50 39.901 20.55 21.03 19.66     ~ 156 0
20 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
21 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
22 GRB 091109B gB 07 30 59.90 -54 05 30.6           ~ 57 0
23 Fermi bn081226044 G 08 02 00.4500 -69 01 49.500           ~ 63 0
24 Fermi bn160408268 gB 08 10 29.93 +71 07 41.7           ~ 45 0
25 GRB 160525B G 09 57 32.2460 +51 12 24.600           ~ 30 0
26 UCAC4 217-047923 * 10 19 02.5992684123 -46 40 11.294771086   13.795 12.458 12.114   ~ 54 0
27 GRB 121226A G 11 14 34.1210 -30 24 22.840           ~ 44 0
28 GRB 211023B G 11 21 14.3110 +39 08 08.360           ~ 32 0
29 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
30 GRB 181123B G 12 17 27.9100 +14 35 52.270           ~ 47 0
31 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
32 GRB 210726A G 12 53 09.8200 +19 11 25.032           ~ 36 0
33 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 198 0
34 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
35 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
36 SDSS J140910.47+275320.8 G 14 09 10.47535 +27 53 20.8393           ~ 279 0
37 GRB 060801 G 14 12 01.2620 +16 58 55.970           ~ 172 0
38 GRB 150423A gB 14 46 18.96 +12 17 00.6           ~ 79 0
39 GRB 120804A G 15 35 47.5100 -28 46 56.110           ~ 99 0
40 GRB 160601A G 15 39 43.9490 +64 32 30.604           ~ 34 0
41 GRB 140903A G 15 52 03.2650 +27 36 10.710           ~ 138 0
42 Fermi bn180402406 gB 16 47 43.90 -14 58 12.1           ~ 31 0
43 GRB 160927A gB 17 04 58.19 +17 19 55.3           ~ 34 0
44 GRB 080919 gB 17 40 53.00 -42 22 29.5           ~ 49 0
45 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
46 Fermi bn130515056 gB 18 53 45.65 -54 16 45.0           ~ 55 0
47 GRB 111020A gB 19 08 12.53 -38 00 43.0           ~ 66 0
48 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
49 GRB 221009A gB 19 13 03.85 +19 46 22.7           ~ 433 0
50 GRB 080702A gB 20 52 12.21 +72 18 46.7           ~ 47 0
51 Fermi bn090621922 gB 20 53 49.30 +69 02 02.9           ~ 65 0
52 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
53 GRB 140129B G 21 47 01.6490 +26 12 23.270           ~ 30 0
54 GRB 070429B G 21 52 03.6910 -38 49 42.820           ~ 125 0
55 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
56 GRB 110112A gB 21 59 43.77 +26 27 24.4           ~ 47 0
57 GRB 170428A G 22 00 18.7100 +26 54 56.280           ~ 52 0
58 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
59 GRB 231117A gB 22 09 37.00 +13 30 58.1           ~ 54 0
60 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
61 GRB 080123 gB 22 35 46.100 -64 54 03.24           ~ 98 0
62 Fermi bn160411062 G 23 17 25.3550 -40 14 30.560           ~ 34 0
63 GRB 120630A gB 23 29 10.75 +42 33 17.4           ~ 19 0

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