2013MNRAS.436.3640L


Query : 2013MNRAS.436.3640L

2013MNRAS.436.3640L - Mon. Not. R. Astron. Soc., 436, 3640-3655 (2013/December-3)

Are gamma-ray bursts the same at high redshift and low redshift ?

LITTLEJOHNS O.M., TANVIR N.R., WILLINGALE R., EVANS P.A., O'BRIEN P.T. and LEVAN A.J.

Abstract (from CDS):

The majority of Swift gamma-ray bursts (GRBs) observed at z ≳ 6 have prompt durations of T90 ≲ 30s, which, at first sight, is surprising given that cosmological time dilation means this corresponds to ≲ 5s in their rest frames. We have tested whether the high-redshift GRBs are consistent with being drawn from the same population as those observed at low redshift by comparing them to an artificially redshifted sample of 114 z < 4 bursts. This is accomplished using two methods to produce realistic high-z simulations of light curves based on the observed characteristics of the low-z sample. In Method 1 we use the Swift/Burst Alert Telescope (BAT) data directly, taking the photons detected in the harder bands to predict what would be seen in the softest energy band if the burst were seen at higher z. In Method 2 we fit the light curves with a model, and use that to extrapolate the expected behaviour over the whole BAT energy range at any redshift. Based on the results of Method 2, a Kolmogorov-Smirnov test of their durations finds a ∼ 1 per cent probability that the high-z GRB sample is drawn from the same population as the bright low-z sample. Although apparently marginally significant, we must bear in mind that this test was partially a posteriori, since the rest-frame short durations of several high-z bursts motivated the study in the first instance.

Abstract Copyright: © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2013)

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

Simbad objects: 25

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Number of rows : 25
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 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
2 Fermi bn100814160 gB 01 29 53.61 -17 59 43.6           ~ 219 0
3 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
4 GRB 100905A gB 02 06 12.06 +14 55 45.9           ~ 45 0
5 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
6 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
7 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 213 0
8 GRB 110422A gB 07 28 11.21 +75 06 24.0           ~ 113 0
9 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
10 GRB 110503A gB 08 51 06.31 +52 12 27.7           ~ 115 0
11 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
12 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
13 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
14 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
15 GRB 090429B gB 14 02 40.10 +32 10 14.6           ~ 166 0
16 GRB 120521C gB 14 17 09.10 +42 08 39.8           ~ 93 0
17 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
18 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
19 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 185 0
20 GRB 080319C gB 17 15 55.48 +55 23 31.7           ~ 174 0
21 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
22 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
23 GRB 120923A gB 20 15 10.73 +06 13 16.9           ~ 59 0
24 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
25 GRB 041228 gB 22 26.6 +05 03           ~ 23 0

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