2020MNRAS.495.4782O


Query : 2020MNRAS.495.4782O

2020MNRAS.495.4782O - Mon. Not. R. Astron. Soc., 495, 4782-4799 (2020/July-2)

Constraints on the circumburst environments of short gamma-ray bursts.

O'CONNOR B., BENIAMINI P. and KOUVELIOTOU C.

Abstract (from CDS):

Observational follow up of well localized short gamma-ray bursts (SGRBs) has left 20g-¡30 per cent of the population without a coincident host galaxy association to deep optical and NIR limits (>=26 mag). These SGRBs have been classified as observationally hostless due to their lack of strong host associations. It has been argued that these hostless SGRBs could be an indication of the large distances traversed by the binary neutron star system (due to natal kicks) between its formation and its merger (leading to an SGRB). The distances of GRBs from their host galaxies can be indirectly probed by the surrounding circumburst densities. We show that a lower limit on those densities can be obtained from early afterglow light curves. We find that ≲16 per cent of short GRBs in our sample took place at densities <=10–4 cm–3. These densities represent the expected range of values at distances greater than the host galaxy's virial radii. We find that out of the five SGRBs in our sample that have been found to be observationally hostless, none are consistent with having occurred beyond the virial radius of their birth galaxies. This implies one of two scenarios. Either these observationally hostless SGRBs occurred outside of the half-light radius of their host galaxy, but well within the galactic halo, or in host galaxies at moderate to high redshifts (z >= 2) that were missed by follow-up observations.

Abstract Copyright: © 2020 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

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

Simbad objects: 58

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Number of rows : 58
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 140930B gB 00 25 23.40 +24 17 41.7           ~ 52 0
2 Fermi bn111117510 gB 00 50 46.220 +23 00 39.22           ~ 141 0
3 GRB 100625A gB 01 03 10.98 -39 05 18.3           ~ 124 0
4 GRB 151127A gB 01 17 54.58 -82 46 15.0           ~ 18 0
5 Fermi bn170127634 gB 01 19 54.47 -30 21 28.6           ~ 36 0
6 GRB 080426 gB 01 45 59.79 +69 28 06.0           ~ 50 0
7 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
8 Fermi bn081024245 gB 01 51 33.80 +61 21 08.2           ~ 75 0
9 GRB 141212A G 02 36 29.9570 +18 08 47.228           ~ 70 0
10 GRB 120305A gB 03 10 08.73 +28 29 30.9           ~ 56 0
11 Fermi bn130912358 gB 03 10 25.60 +13 59 55.7           ~ 57 0
12 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
13 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
14 GRB 060313 G 04 26 28.4020 -10 50 39.901 20.55 21.03 19.66     ~ 156 0
15 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
16 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
17 GRB 091109B gB 07 30 59.90 -54 05 30.6           ~ 57 0
18 Fermi bn081226044 G 08 02 00.4500 -69 01 49.500           ~ 63 0
19 Fermi bn160408268 gB 08 10 29.93 +71 07 41.7           ~ 45 0
20 GRB 160525B G 09 57 32.2460 +51 12 24.600           ~ 30 0
21 UCAC4 217-047923 * 10 19 02.5992684123 -46 40 11.294771086   13.795 12.458 12.114   ~ 54 0
22 GRB 090515 gB 10 56 41.0 +14 27 22           ~ 122 0
23 GRB 121226A G 11 14 34.1210 -30 24 22.840           ~ 44 0
24 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
25 GRB 181123B G 12 17 27.9100 +14 35 52.270           ~ 47 0
26 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
27 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 198 0
28 NGC 4993 Sy2 13 09 47.6908761600 -23 23 02.314044636   13.34   11.92   ~ 397 0
29 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
30 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
31 GRB 060801 G 14 12 01.2620 +16 58 55.970           ~ 172 0
32 GRB 150423A gB 14 46 18.96 +12 17 00.6           ~ 79 0
33 GRB 120804A G 15 35 47.5100 -28 46 56.110           ~ 99 0
34 GRB 160601A G 15 39 43.9490 +64 32 30.604           ~ 34 0
35 GRB 140903A G 15 52 03.2650 +27 36 10.710           ~ 138 0
36 GRB 090305 G 16 07 07.5960 -31 33 22.540           ~ 53 0
37 Fermi bn150301045 gB 16 17 13.13 -48 42 47.2           ~ 31 0
38 Fermi bn180402406 gB 16 47 43.90 -14 58 12.1           ~ 31 0
39 GRB 160927A gB 17 04 58.19 +17 19 55.3           ~ 34 0
40 GRB 080919 gB 17 40 53.00 -42 22 29.5           ~ 49 0
41 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
42 Fermi bn130515056 gB 18 53 45.65 -54 16 45.0           ~ 55 0
43 GRB 080503 gB 19 06 28.74 +68 47 35.8           ~ 172 0
44 GRB 111020A gB 19 08 12.53 -38 00 43.0           ~ 66 0
45 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
46 Fermi bn131004904 gB 19 44 27.20 -02 57 31.0           ~ 113 0
47 GRB 080702A gB 20 52 12.21 +72 18 46.7           ~ 47 0
48 Fermi bn090621922 gB 20 53 49.30 +69 02 02.9           ~ 65 0
49 GRB 140129B G 21 47 01.6490 +26 12 23.270           ~ 30 0
50 GRB 070429B G 21 52 03.6910 -38 49 42.820           ~ 125 0
51 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
52 GRB 110112A gB 21 59 43.77 +26 27 24.4           ~ 47 0
53 GRB 170428A G 22 00 18.7100 +26 54 56.280           ~ 52 0
54 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
55 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
56 GRB 080123 gB 22 35 46.100 -64 54 03.24           ~ 98 0
57 Fermi bn160411062 G 23 17 25.3550 -40 14 30.560           ~ 34 0
58 GRB 120630A gB 23 29 10.75 +42 33 17.4           ~ 19 0

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