2025A&A...699A.113G


Query : 2025A&A...699A.113G

2025A&A...699A.113G - Astronomy and Astrophysics, volume 699A113 (2025/7-1)

Binary neutron star merger offsets from their host galaxies II. Short-duration gamma-ray bursts.

GASPARI N., LEVAN A.J., CHRIMES A.A. and NUGENT A.E.

Abstract (from CDS):

Context. The mergers of binary neutron stars (BNSs) and neutron star-black hole (NSBH) binaries have long been linked to short-duration gamma-ray bursts (SGRBs). However, despite their stellar progenitors, SGRBs are often found outside the stellar light of the host galaxy. This is commonly attributed to supernova kicks, which displace the SGRB progenitors from the original stellar population.
Aims. Our goal is to use stellar population synthesis models to reproduce and interpret the observed offsets of a statistical sample of SGRBs, using realistic galactic models based on the observed host properties.
Methods. We derived the host galaxy potentials from the observed properties on a case-by-case basis and simulated the galactic trajectories of synthetic BNSs and NSBHs from the BPASS code using three different kick prescriptions. We compared predicted and observed offsets to investigate the impact of velocity kicks, host galaxy types, and host association criteria.
Results. The locations of the SGRB population are consistent with the expectations of kicked BNS or BHNS progenitors, implying that such mergers are the dominant (and perhaps the only) progenitor system. Predictions for NSBHs provide a significantly worse fit compared to BNSs, while we find no significant difference when comparing different kick prescriptions. For late-type hosts, we find the best agreement when including hosts with a probability of chance alignment, Pch, of up to 20%, while lower Pch thresholds lead us to overestimate SGRB offsets. We argue that Pch is biased against viable hosts at the largest offsets and suggest the use of less conservative Pch thresholds for late-type hosts. For early-type hosts, the predictions underestimate SGRB offsets in a few cases regardless of the Pch threshold applied. We argue that this is likely due to the models missing galaxy evolution or spurious host associations.

Abstract Copyright: © The Authors 2025

Journal keyword(s): gravitational waves - binaries: close - gamma-ray burst: general - stars: neutron

Simbad objects: 70

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Number of rows : 70
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 bn150120123 G 00 41 16.5630 +33 59 42.598           ~ 70 0
4 Fermi bn100117879 G 00 45 04.6610 -01 35 42.020           ~ 155 0
5 Fermi bn111117510 gB 00 50 46.220 +23 00 39.22           ~ 141 0
6 GRB 100625A gB 01 03 10.98 -39 05 18.3           ~ 124 0
7 Fermi bn170127634 gB 01 19 54.47 -30 21 28.6           ~ 36 0
8 GRB 180805B gB 01 43 07.59 -17 29 36.4           ~ 32 0
9 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
10 GRB 130822A gB 01 51 41.27 -03 12 31.7           ~ 34 0
11 GRB 141212A G 02 36 29.9570 +18 08 47.228           ~ 70 0
12 PSO J047.1631+13.1580 G 03 08 39.14930640 +13 09 29.0253240           ~ 144 0
13 GRB 120305A gB 03 10 08.73 +28 29 30.9           ~ 56 0
14 GRB 200411A gB 03 10 39.39 -52 19 03.3           ~ 31 0
15 GRB 070729 gB 03 45 16.04 -39 19 19.9           ~ 81 0
16 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
17 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
18 GRB 170728A gB 03 55 36 +12 10.0           ~ 22 0
19 Fermi bn161001045 gB 04 47 40.84 -57 15 39.9           ~ 41 0
20 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
21 GRB 161104A gB 05 11 34.45 -51 27 36.3           ~ 28 0
22 GRB 210919A gB 05 21 01.05 +01 18 42.1           ~ 41 0
23 GRB 200907B G 05 56 06.9510 +06 54 22.637           ~ 24 0
24 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
25 Fermi bn160408268 gB 08 10 29.93 +71 07 41.7           ~ 45 0
26 SDSS J093805.33+153719.0 G 09 38 05.33384 +15 37 19.0406           ~ 146 0
27 GRB 160525B G 09 57 32.2460 +51 12 24.600           ~ 30 0
28 GRB 090515 gB 10 56 41.0 +14 27 22           ~ 122 0
29 GRB 121226A G 11 14 34.1210 -30 24 22.840           ~ 44 0
30 GRB 160303A gB 11 14 48.16 +22 44 31.3           ~ 47 0
31 Fermi bn180618030 G 11 19 45.8010 +73 50 15.030           ~ 38 0
32 Fermi bn180418281 G 11 20 29.2100 +24 55 58.734           ~ 57 0
33 GRB 211023B G 11 21 14.3110 +39 08 08.360           ~ 32 0
34 GRB 201221D gB 11 24 14.19 +42 08 35.5           ~ 48 0
35 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
36 GRB 181123B G 12 17 27.9100 +14 35 52.270           ~ 47 0
37 GALEX J123205.0-105600 Bz? 12 32 04.9717245480 -10 56 00.722548932         16.421 ~ 186 0
38 SDSS J123612.87+285858.8 BiC 12 36 12.8803407000 +28 58 58.780075656           ~ 328 1
39 GRB 210726A G 12 53 09.8200 +19 11 25.032           ~ 36 0
40 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
41 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
42 SDSS J140910.47+275320.8 G 14 09 10.47535 +27 53 20.8393           ~ 279 0
43 GRB 060801 G 14 12 01.2620 +16 58 55.970           ~ 172 0
44 GRB 150831A gB 14 44 05.84 -25 38 06.3           ~ 38 0
45 GRB 120804A G 15 35 47.5100 -28 46 56.110           ~ 99 0
46 Fermi bn170728961 G 15 51 55.5290 +70 07 22.038           ~ 54 0
47 GRB 140903A G 15 52 03.2650 +27 36 10.710           ~ 138 0
48 GRB 050813 gB 16 07 57.190 +11 14 57.80           ~ 147 0
49 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
50 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
51 GRB 191031D gB 18 53 09.57 +47 38 38.5           ~ 46 0
52 Fermi bn130515056 gB 18 53 45.65 -54 16 45.0           ~ 55 0
53 PSO J285.9246+45.7134 G 19 03 41.90914320 +45 42 48.4220520           ~ 63 0
54 PSO J292.2283+33.9161 G 19 28 54.81164400 +33 54 58.1227560           ~ 25 0
55 GRB 140622A gB 21 08 41.56 -14 25 09.5           ~ 61 0
56 Fermi bn210323918 G 21 11 47.3200 +25 22 09.989           ~ 44 0
57 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
58 GRB 140129B G 21 47 01.6490 +26 12 23.270           ~ 30 0
59 GRB 070429B G 21 52 03.6910 -38 49 42.820           ~ 125 0
60 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
61 Fermi bn151229285 gB 21 57 28.78 -20 43 55.2           ~ 38 0
62 GRB 170428A G 22 00 18.7100 +26 54 56.280           ~ 52 0
63 GRB 051210 gB 22 00 40.930 -57 36 47.10           ~ 138 0
64 Fermi bn160624477 gB 22 00 46.21 +29 38 37.8           ~ 69 0
65 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
66 GRB 080123 gB 22 35 46.100 -64 54 03.24           ~ 98 0
67 Fermi bn200219317 G 22 50 33.1080 -59 07 11.579           ~ 42 0
68 NVSS J230126-385839 rG 23 01 26.7650 -38 58 40.422   22.22 21.22 21   ~ 325 1
69 GRB 180727A G 23 06 40.0380 -63 03 07.088           ~ 29 0
70 Fermi bn160411062 G 23 17 25.3550 -40 14 30.560           ~ 34 0

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