2020ApJ...889..110K


Query : 2020ApJ...889..110K

2020ApJ...889..110K - Astrophys. J., 889, 110-110 (2020/February-1)

Systematic study of the peak energy of broadband gamma-ray Burst spectra.

KATSUKURA D., SAKAMOTO T., TASHIRO M.S. and TERADA Y.

Abstract (from CDS):

We have performed a systematic study of gamma-ray bursts (GRBs), which have various values in the peak energy of the νFν spectrum of prompt emission, Epeak, observed by the Swift/Burst Alert Telescope (BAT) and Fermi/Gamma-ray Burst Monitor, investigating their prompt and X-ray afterglow emissions. We cataloged long-lasting GRBs observed by Swift between 2004 December and 2014 February in three categories according to the classification by Sakamoto et al.: X-ray flashes (XRFs), X-ray-rich GRBs (XRRs), and classical GRBs (C-GRBs). We then derived Epeakobs, as well as Epeaksrc if viable, of the Swift spectra of their prompt emission. We also analyzed their X-ray afterglows and found that GRB events with a lower Epeaksrc, i.e., softer GRBs, are fainter in 0.3-10 keV X-ray luminosity and decay more slowly than harder GRBs. The intrinsic event rates of the XRFs, XRRs, and C-GRBs were calculated using the Swift/BAT trigger algorithm. Those of the XRRs and XRFs are larger than that of the C-GRBs. If we assume that the observational diversity of Epeak is explained using the off-axis model, these results yield a jet half-opening angle of Δθ ∼ 0.°3, and a variance of the observing angles θobs <= 0.°6. This implies that this tiny variance would be responsible for the Epeak diversity observed by Swift/BAT, which is unrealistic. Therefore, we conclude that the Epeak diversity is not explained with the off-axis model, but is likely to originate from some intrinsic properties of the jets.

Abstract Copyright: © 2020. The American Astronomical Society. All rights reserved.

Journal keyword(s): Gamma-ray bursts - High energy astrophysics - Jets - Relativistic jets

CDS comments: Not all XRFs and XRRs are in SIMBAD (no coordinates given).

Simbad objects: 31

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Number of rows : 31
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 050824 gB 00 48 56.100 +22 36 32.00 19.66 21.03 20.46 23.70   ~ 184 0
2 GRB 060825 gB 01 12 29.520 +55 47 51.59           ~ 49 0
3 GRB 081222 gB 01 30 57.76 -34 05 44.0           ~ 199 0
4 GRB 050406 gB 02 17 52.200 -50 11 15.81     18.83     ~ 125 0
5 Fermi bn090926914 gB 03 05 14.30 -38 59 50.9           ~ 149 1
6 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
7 GRB 131229A gB 05 40 55.61 -04 23 46.6           ~ 35 0
8 GRB 081121 gB 05 57 07.70 -60 36 42.1           ~ 152 0
9 GRB 050410 gB 05 59 13.460 +79 36 12.00           ~ 53 0
10 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
11 GRB 080714 gB 12 32 25.29 -60 16 40.2           ~ 54 0
12 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
13 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
14 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
15 GRB 050915B gB 14 36 25.890 -67 24 33.21           ~ 56 0
16 GRB 060428B gB 15 41 25.570 +62 01 28.93 20.64 20.62 19.50     ~ 71 0
17 GRB 060923B gB 15 52 46.740 -30 54 11.30 19.80         ~ 41 0
18 GRB 060219 gB 16 07 21.520 +32 18 57.59           ~ 50 0
19 Fermi bn121011469 gB 17 20 51.27 +41 06 36.8           ~ 55 0
20 GRB 060926 gB 17 35 43.660 +13 02 18.60     19.36     ~ 135 0
21 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
22 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
23 GRB 110625A gB 19 06 55.85 +06 45 19.2           ~ 69 0
24 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
25 Fermi bn110610640 gB 20 32 42.97 +74 49 31.2           ~ 37 0
26 Fermi bn080804972 gB 21 54 41.90 -53 11 20.2           ~ 158 0
27 GRB 060927A gB 21 58 11.930 +05 21 50.32           ~ 215 0
28 Fermi bn080916406 gB 22 25 09.30 -57 01 33.7           ~ 177 0
29 Fermi bn100816026 gB 23 26 57.56 +26 34 42.6           ~ 170 0
30 GRB 060707 gB 23 48 19.000 -17 54 17.00     19.79     ~ 170 0
31 GRB 050819 gB 23 55 01.650 +24 51 38.80           ~ 75 0

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