2022MNRAS.515.2591C


Query : 2022MNRAS.515.2591C

2022MNRAS.515.2591C - Mon. Not. R. Astron. Soc., 515, 2591-2611 (2022/September-2)

Towards an understanding of long gamma-ray burst environments through circumstellar medium population synthesis predictions.

CHRIMES A.A., GOMPERTZ B.P., KANN D.A., VAN MARLE A.J., ELDRIDGE J.J., GROOT P.J., LASKAR T., LEVAN A.J., NICHOLL M., STANWAY E.R. and WIERSEMA K.

Abstract (from CDS):

The temporal and spectral evolution of gamma-ray burst (GRB) afterglows can be used to infer the density and density profile of the medium through which the shock is propagating. In long-duration (core-collapse) GRBs, the circumstellar medium (CSM) is expected to resemble a wind-blown bubble, with a termination shock, separating the stellar wind and the interstellar medium (ISM). A long standing problem is that flat density profiles, indicative of the ISM, are often found at lower radii than expected for a massive star progenitor. Furthermore, the presence of both wind-like environments at high radii and ISM-like environments at low radii remains a mystery. In this paper, we perform a 'CSM population synthesis' with long GRB progenitor stellar evolution models. Analytic results for the evolution of wind blown bubbles are adjusted through comparison with a grid of 2D hydrodynamical simulations. Predictions for the emission radii, ratio of ISM to wind-like environments, wind, and ISM densities are compared with the largest sample of afterglow derived parameters yet compiled, which we make available for the community. We find that high ISM densities of n ∼ 1000 cm–3 best reproduce observations. If long GRBs instead occur in typical ISM densities of n ∼ 1 cm–3, then the discrepancy between theory and observations is shown to persist at a population level. We discuss possible explanations for the origin of variety in long GRB afterglows, and for the overall trend of CSM modelling to over-predict the termination shock radius.

Abstract Copyright: © 2022 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): γ-ray burst: general - stars: winds, outflows - stars: Wolf-Rayet ;

Simbad objects: 90

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Number of rows : 90
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 180720B gB 00 02 06.99 -02 55 07.8           ~ 215 0
2 GRB 150910A gB 00 22 40.14 +33 28 22.4           ~ 79 0
3 GRB 071031 gB 00 25 37.40 -58 03 33.9           ~ 184 0
4 GRB 080710 gB 00 33 05.68 +19 30 05.8           ~ 136 0
5 SN 2010ma SN* 00 48 55.35 -34 33 59.5           SNIc 190 1
6 GRB 050824 gB 00 48 56.100 +22 36 32.00 19.66 21.03 20.46 23.70   ~ 184 0
7 Fermi bn120729456 gB 00 52 17.84 +49 56 23.1           ~ 122 0
8 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
9 GRB 050908 gB 01 21 50.750 -12 57 17.20           ~ 179 0
10 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
11 Fermi bn091208410 gB 01 57 38.50 +16 52 50.7           ~ 220 0
12 GRB 091018 gB 02 08 46 -57 33.0           ~ 169 0
13 GRB 110918A gB 02 10 09.39 -27 06 19.6           ~ 83 0
14 GRB 071112C gB 02 36 50.89 +28 22 16.9           ~ 164 0
15 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
16 SN 2013ez SN* 02 53 56.70 +13 23 13.6           ~ 118 0
17 GRB 140801A gB 02 56 16.50 +30 56 16.8           ~ 55 0
18 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
19 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 315 1
20 GRB 050318 gB 03 18 51.000 -46 23 43.61 18.10 18.68 17.58     ~ 189 0
21 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 208 0
22 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 168 0
23 GRB 121024A gB 04 41 53.31 -12 17 26.1           ~ 143 0
24 GRB 060124 gB 05 08 25.900 +69 44 26.98   18.91 17.35     ~ 280 0
25 GRB 061126 gB 05 46 24.460 +64 12 38.49 18.62 18.79 19.20     ~ 182 1
26 GRB 090328 gB 06 02 39.69 -41 52 55.1           ~ 194 1
27 Fermi bn080928628 gB 06 20 16.85 -55 11 59.3           ~ 187 0
28 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
29 GRB 140430A gB 06 51 44.58 +23 01 25.5           ~ 81 0
30 GRB 070125 gB 07 51 17.80 +31 09 04.8           ~ 188 0
31 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
32 GRB 140419A gB 08 27 57.56 +46 14 25.3           ~ 95 0
33 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
34 GRB 050505 gB 09 27 03.300 +30 16 23.70     20.74     ~ 206 0
35 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
36 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
37 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
38 GRB 100219A gB 10 16 48.48 -12 34 00.0           ~ 130 0
39 GRB 180325A gB 10 29 42.57 +24 27 48.7           ~ 85 0
40 GRB 110205A gB 10 58 31.12 +67 31 31.2           ~ 213 0
41 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
42 GRB 140515A gB 12 24 15.48 +15 06 17.7           ~ 90 0
43 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
44 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 244 1
45 GRB 060512 gB 13 03 05.810 +41 11 27.21 19.12 19.63 17.20     ~ 142 0
46 Fermi bn140423356 gB 13 09 06.20 +49 50 18.3           ~ 114 0
47 GRB 090313 gB 13 13 36.00 +08 05 10.7           ~ 149 0
48 GRB 050801 gB 13 36 35.000 -21 55 41.00 15.03 15.82 15.46     ~ 164 0
49 GRB 140311A gB 13 57 13.29 +00 38 31.7           ~ 86 0
50 GRB 120521C gB 14 17 09.10 +42 08 39.8           ~ 93 0
51 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
52 GRB 050802 gB 14 37 05.820 +27 47 12.62 16.85 17.38 16.97     ~ 186 0
53 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 214 0
54 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 180 0
55 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
56 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
57 GRB 120404A gB 15 40 02.29 +12 53 06.3           ~ 104 0
58 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
59 GRB 110715A gB 15 50 44.090 -46 14 06.53           ~ 120 0
60 GRB 120327A gB 16 27 27.49 -29 24 53.8           ~ 116 0
61 GRB 140629A gB 16 35 54.44 +41 52 36.7           ~ 89 0
62 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 185 0
63 GRB 080210 gB 16 45 04.03 +13 49 36.3           ~ 121 0
64 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 198 0
65 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
66 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
67 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
68 Fermi bn140506880 gB 18 27 06.04 -55 38 08.7           ~ 113 0
69 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
70 GRB 080603A gB 18 37 37.95 +62 44 39.6           ~ 89 0
71 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
72 GRB 110726A gB 19 06 52.21 +56 04 16.4           ~ 55 0
73 GRB 071010A gB 19 12 14.42 -32 24 06.2           ~ 138 0
74 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 181 0
75 GRB 120923A gB 20 15 10.73 +06 13 16.9           ~ 59 0
76 GRB 050315 gB 20 25 54.100 -42 36 02.19           ~ 225 0
77 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 235 0
78 GRB 161023A gB 20 44 05.20 -47 39 48.7           ~ 49 0
79 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 204 0
80 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
81 GRB 080413B gB 21 44 34.62 -19 58 51.2           ~ 191 0
82 iPTF 14bfu SN* 21 52 30.00 +32 00 52.5           SNIc 80 0
83 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
84 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
85 Fermi bn091024380 gB 22 37 +56.9           ~ 151 0
86 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1
87 GRB 131030A gB 23 00 16.14 -05 22 05.2           ~ 126 0
88 GRB 081029 gB 23 07 06 -68 10.7           ~ 121 0
89 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0
90 SN 2013fu SN* 23 54 29.91 +29 25 47.6           SNIb/c 144 1

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