2018ApJ...866..162G


Query : 2018ApJ...866..162G

2018ApJ...866..162G - Astrophys. J., 866, 162-162 (2018/October-3)

The environments of the most energetic gamma-ray bursts.

GOMPERTZ B.P., FRUCHTER A.S. and PE'ER A.

Abstract (from CDS):

We analyze the properties of a sample of long gamma-ray bursts (LGRBs) detected by the Fermi satellite that have a spectroscopic redshift and good follow-up coverage at both X-ray and optical/near infrared wavelengths. The evolution of LGRB afterglows depends on the density profile of the external medium, enabling us to separate wind or interstellar medium (ISM)-like environments based on the observations. We do this by identifying the environment that provides the best agreement between estimates of p, the index of the underlying power-law distribution of electron energies, as determined by the behavior of the afterglow in different spectral/temporal regimes. At 11 rest-frame hours after trigger, we find a roughly even split between ISM-like and wind-like environments. We further find a 2σ separation in the prompt emission energy distributions of wind-like and ISM-like bursts. We investigate the underlying physical parameters of the shock, and calculate the (degenerate) product of density and magnetic field energy (εB). We show that εB must be ≪10–2 to avoid implied densities comparable to the intergalactic medium. Finally, we find that the most precisely constrained observations disagree on p by more than would be expected based on observational errors alone. This suggests additional sources of error that are not incorporated in the standard afterglow theory. For the first time, we provide a measurement of this intrinsic error that can be represented as an error in the estimate of p of magnitude 0.25 ± 0.04. When this error is included in the fits, the number of LGRBs with an identified environment drops substantially, but the equal division between the two types remains.

Abstract Copyright: © 2018. The American Astronomical Society. All rights reserved.

Journal keyword(s): gamma-ray burst: general

Simbad objects: 56

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Number of rows : 56
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 bn131231198 gB 00 42 44.0 -01 29 40           ~ 103 0
2 SN 2010ma SN* 00 48 55.35 -34 33 59.5           SNIc 190 1
3 Fermi bn140703026 gB 00 51 58.99 +45 06 05.4           ~ 90 0
4 Fermi bn120729456 gB 00 52 17.84 +49 56 23.1           ~ 122 0
5 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
6 Fermi bn091208410 gB 01 57 38.50 +16 52 50.7           ~ 220 0
7 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
8 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
9 GRB 140801A gB 02 56 16.50 +30 56 16.8           ~ 55 0
10 GRB 140907A gB 03 12 34.98 +46 36 17.2           ~ 81 0
11 Fermi bn170113420 gB 04 06 59 -71 56.0           ~ 64 0
12 Fermi bn150514774 gB 04 59 30.45 -60 58 07.0           ~ 51 0
13 Fermi bn141004973 gB 05 06 56.11 +12 49 10.1           ~ 75 0
14 Fermi bn100728095 gB 05 55 02.00 -15 15 20.2           ~ 157 0
15 Fermi bn150301818 gB 05 56 40.04 -57 58 10.4           ~ 67 0
16 GRB 081121 gB 05 57 07.70 -60 36 42.1           ~ 152 0
17 GRB 090328 gB 06 02 39.69 -41 52 55.1           ~ 194 1
18 Fermi bn120711115 gB 06 18 42.839 -70 59 56.78           ~ 125 0
19 GRB 140213A gB 07 00 37.18 -73 08 14.1           ~ 102 0
20 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
21 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 193 0
22 Fermi bn150314205 gB 08 26 40.82 +63 50 03.4           ~ 117 0
23 Fermi bn161017745 gB 09 31 04.53 +43 07 35.0           ~ 75 0
24 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
25 Fermi bn111228657 gB 10 00 16.04 +18 17 52.2           ~ 201 0
26 GRB 131108A gB 10 26 00.480 +09 39 44.05           ~ 96 0
27 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
28 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
29 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
30 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 244 1
31 Fermi bn100414097 gB 12 48 30.0 +08 41 35           ~ 136 0
32 Fermi bn121211574 gB 13 02 07.99 +30 08 54.6           ~ 99 0
33 Fermi bn130420313 gB 13 04 25.49 +59 25 26.8           ~ 112 0
34 Fermi bn140423356 gB 13 09 06.20 +49 50 18.3           ~ 114 0
35 Fermi bn120811649 gB 13 18 43.82 +62 18 02.8           ~ 113 0
36 GRB 130907A gB 14 23 34.03 +45 36 27.1           ~ 120 0
37 Fermi bn160804065 gB 14 46 31.20 +09 59 56.1           ~ 79 0
38 GRB 091003A gB 16 46 04.680 +36 37 31.08           ~ 135 0
39 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
40 Fermi bn151027166 gB 18 09 56.87 +61 21 12.3           ~ 143 0
41 Fermi bn140506880 gB 18 27 06.04 -55 38 08.7           ~ 113 0
42 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
43 Fermi bn140620219 gB 18 47 29.00 +49 43 51.0           ~ 37 0
44 Fermi bn140512814 gB 19 17 28.81 -15 05 39.5           ~ 133 0
45 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
46 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 235 0
47 GRB 150403A gB 20 46 01.17 -62 42 40.1           ~ 116 0
48 Fermi bn160509374 gB 20 47 00.90 +76 06 30.1           ~ 141 0
49 GRB 160623A gB 21 01 11.54 +42 13 15.5           ~ 73 0
50 GRB 141028A gB 21 30 24.46 -00 13 55.6           ~ 109 0
51 iPTF 14bfu SN* 21 52 30.00 +32 00 52.5           SNIc 80 0
52 Fermi bn080916406 gB 22 25 09.30 -57 01 33.7           ~ 177 0
53 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1
54 Fermi bn150821406 gB 22 47 39.15 -57 53 38.2           ~ 71 0
55 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0
56 GRB 130518A gB 23 42 39.79 +47 27 55.2           ~ 86 0

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