2015MNRAS.454.1785T


Query : 2015MNRAS.454.1785T

2015MNRAS.454.1785T - Mon. Not. R. Astron. Soc., 454, 1785-1791 (2015/December-1)

Research on the redshift evolution of luminosity function and selection effect of GRBs.

TAN W.-W. and WANG F.Y.

Abstract (from CDS):

We study the redshift evolution of the luminosity function (LF) and redshift selection effect of long gamma-ray bursts (LGRBs). The method is to fit the observed peak flux and redshift distributions, simultaneously. To account for the complex triggering algorithm of Swift, we use a flux triggering efficiency function. We find evidence supporting an evolving LF, where the break luminosity scales as Lb ∝ (1 + z)τ, with τ=3.5^+0.4_-0.2 and 0.8^+0.1_-0.08 for two kinds of LGRB rate models. The corresponding local GRB rates are {dot}R(0)=0.86^+0.11_-0.08  yr^-1 Gpc^-3 and 0.54^+0.25_-0.07  yr^-1 Gpc^-3, respectively. Furthermore, by comparing the redshift distribution between the observed one and our mocked one, we find that the redshift detection efficiency of the flux triggered GRBs decreases with redshift. Especially, a great number of GRBs miss their redshifts in the redshift range of 1 < z < 2.5, where `redshift desert' effect may be dominated. More interestingly, our results show that the `redshift desert' effect is mainly introduced by the dimmer GRBs, e.g. P < 10- 7ergs- 1cm- 2, but has no effect on the brighter GRBs.

Abstract Copyright: © 2015 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2015)

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

Simbad objects: 34

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Number of rows : 34
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 101225A gB 00 00 47.48 +44 36 01.0           ~ 163 0
2 GRB 050911A gB 00 54 38.290 -38 50 58.50           ~ 66 0
3 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
4 GRB 141026A gB 02 56 20.29 +26 55 42.4           ~ 60 0
5 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
6 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
7 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
8 GRB 121027A gB 04 14 23.450 -58 49 47.17           ~ 136 0
9 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 213 0
10 GRB 060116 gB 05 38 46.170 -05 26 15.08           ~ 86 0
11 SN 2010bh SN* 07 10 30.63 -56 15 19.7           SNIc 336 1
12 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
13 GRB 051227 gB 08 20 58.107 +31 55 32.01           ~ 127 0
14 GRB 090916 gB 08 26 19.60 +25 56 27.3           ~ 29 0
15 GRB 051016B gB 08 48 27.810 +13 39 20.00 20.45         ~ 153 0
16 SDSS J093805.33+153719.0 G 09 38 05.33384 +15 37 19.0406           ~ 146 0
17 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
18 Fermi bn100216422 gB 10 17 03 +35 31.0           ~ 32 0
19 GRB 140515A gB 12 24 15.48 +15 06 17.7           ~ 90 0
20 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
21 GRB 090607 gB 12 44 46.70 +44 06 28.4           ~ 40 0
22 GRB 090429B gB 14 02 40.10 +32 10 14.6           ~ 166 0
23 GRB 051114A gB 15 05 03.8 +60 09 22           ~ 29 0
24 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
25 GRB 090715B gB 16 45 21.59 +44 50 20.1           ~ 144 0
26 GRB 090531B gB 16 48 15.0 -36 01 27           ~ 58 0
27 GRB 080520 gB 18 40 46.50 -54 59 30.4           ~ 68 0
28 GRB 080503 gB 19 06 28.74 +68 47 35.8           ~ 172 0
29 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
30 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
31 GRB 060505 gB 22 07 03.440 -27 48 51.89           ~ 286 1
32 GRB 080123 gB 22 35 46.100 -64 54 03.24           ~ 98 0
33 GRB 100213A gB 23 17 34.04 +43 22 44.1           ~ 31 0
34 Fermi bn100816026 gB 23 26 57.56 +26 34 42.6           ~ 170 0

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