2016ApJ...831...28T


Query : 2016ApJ...831...28T

2016ApJ...831...28T - Astrophys. J., 831, 28-28 (2016/November-1)

Investigating the impact of optical selection effects on observed rest-frame prompt GRB properties.

TURPIN D., HEUSSAFF V., DEZALAY J.-P., ATTEIA J.-L., KLOTZ A. and DORNIC D.

Abstract (from CDS):

Measuring gamma-ray burst (GRB) properties in their rest frame is crucial for understanding the physics at work in GRBs. This can only be done for GRBs with known redshifts. Since redshifts are usually measured from the optical spectrum of the afterglow, correlations between prompt and afterglow emissions may introduce biases into the distribution of the rest-frame properties of the prompt emission, especially considering that we measure the redshift of only one-third of Swift GRBs. In this paper, we study the optical flux of GRB afterglows and its connection to various intrinsic properties of GRBs. We also discuss the impact of the optical selection effect on the distribution of rest-frame prompt properties of GRBs. Our analysis is based on a sample of 90 GRBs with good optical follow-up and well-measured prompt emission. Seventy-six of them have a measure of redshift and 14 have no redshift. We compare the rest-frame prompt properties of GRBs with different afterglow optical fluxes in order to check for possible correlations between the promt properties and the optical flux of the afterglow. The optical flux is measured two hours after the trigger, which is a typical time for the measure of the redshift. We find that the optical flux of GRB afterglows in our sample is mainly driven by their optical luminosity and depends only slightly on their redshift. We show that GRBs with low and high afterglow optical fluxes have similar Epi, Eiso, and Liso, indicating that the rest-frame distributions computed from GRBs with a redshift are not significantly distorted by optical selection effects. However, we found that the T90rest distribution is not immune to optical selection effects, which favor the selection of GRBs with longer durations. Finally, we note that GRBs well above the Epi-Eiso relation have lower optical fluxes and we show that optical selection effects favor the detection of GRBs with bright optical afterglows located close to or below the best-fit Epi-Eiso relation (Amati relation), whose redshift is easily measurable. With more than 300 GRBs with a redshift, we now have a much better view of the intrinsic properties of these remarkable events. At the same time, increasing statistics allow us to understand the biases acting on the measurements. The optical selection effects induced by the redshift measurement strategies cannot be neglected when we study the properties of GRBs in their rest frame, even for studies focused on prompt emission.

Abstract Copyright: © 2016. The American Astronomical Society. All rights reserved.

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

Simbad objects: 91

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Number of rows : 91
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 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
2 Fermi bn131231198 gB 00 42 44.0 -01 29 40           ~ 103 0
3 Fermi bn140703026 gB 00 51 58.99 +45 06 05.4           ~ 90 0
4 GRB 041006 gB 00 54 50.17 +01 14 07.0           ~ 202 2
5 Fermi bn100814160 gB 01 29 53.61 -17 59 43.6           ~ 219 0
6 GRB 081222 gB 01 30 57.76 -34 05 44.0           ~ 199 0
7 Fermi bn091208410 gB 01 57 38.50 +16 52 50.7           ~ 220 0
8 GRB 040924 gB 02 06 22.52 +16 08 48.8           ~ 169 1
9 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
10 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
11 GRB 080411 gB 02 31 54.82 -71 18 07.5           ~ 109 0
12 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
13 Fermi bn100728439 gB 02 56 13.44 +00 16 51.6           ~ 142 0
14 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 315 1
15 Fermi bn101011707 gB 03 13 10.62 -65 58 55.6           ~ 48 0
16 GRB 060115 gB 03 36 08.400 +17 20 43.00           ~ 179 0
17 Fermi bn091221870 gB 03 43 11.40 +23 14 28.0           ~ 66 0
18 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 168 0
19 Fermi bn120907017 gB 04 58 59.99 -09 18 53.7           ~ 89 0
20 GRB 140626A gB 05 09 31.22 -82 37 51.0           ~ 18 0
21 GRB 081121 gB 05 57 07.70 -60 36 42.1           ~ 152 0
22 GRB 141017A gB 06 14 31.18 -58 34 56.5           ~ 26 0
23 GRB 140213A gB 07 00 37.18 -73 08 14.1           ~ 102 0
24 GRB 110422A gB 07 28 11.21 +75 06 24.0           ~ 113 0
25 GRB 071020 gB 07 58 39.65 +32 51 38.8           ~ 158 0
26 GRB 070612A gB 08 05 28.530 +37 16 09.57           ~ 82 0
27 SN 2002lt SN* 08 08 59.858 +06 43 37.52           SNIc: 363 1
28 GRB 140419A gB 08 27 57.56 +46 14 25.3           ~ 95 0
29 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
30 GRB 110503A gB 08 51 06.31 +52 12 27.7           ~ 115 0
31 GRB 130408A gB 08 57 37.30 -32 21 38.9           ~ 98 0
32 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
33 GRB 130505A gB 09 17 21.9014988888 +01 42 03.426207768           ~ 94 0
34 Fermi bn090519881 gB 09 29 16.20 +00 11 23.9           ~ 98 0
35 GRB 020124 gB 09 32 50.8 -11 31 11           ~ 155 0
36 Fermi bn140709637 gB 09 44 13.20 +63 31 46.5           ~ 28 0
37 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
38 GRB 071010B gB 10 02 09.20 +45 43 52.2           ~ 173 0
39 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
40 GRB 110205A gB 10 58 31.12 +67 31 31.2           ~ 213 0
41 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
42 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
43 GRB 030328 gB 12 10 48.4 -09 20 51           ~ 148 0
44 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
45 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
46 Fermi bn121211574 gB 13 02 07.99 +30 08 54.6           ~ 99 0
47 Fermi bn130420313 gB 13 04 25.49 +59 25 26.8           ~ 112 0
48 Fermi bn140423356 gB 13 09 06.20 +49 50 18.3           ~ 114 0
49 Fermi bn120811649 gB 13 18 43.82 +62 18 02.8           ~ 113 0
50 GRB 051008 gB 13 31 28.100 +42 08 05.01 17.06   14.11     ~ 90 0
51 GRB 990510 gB 13 38 07.64 -80 29 48.8           ~ 499 1
52 GRB 090429B gB 14 02 40.10 +32 10 14.6           ~ 166 0
53 Fermi bn140102887 gB 14 07 40.65 +01 19 59.8           ~ 53 0
54 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
55 Fermi bn140808038 gB 14 44 53.27 +49 12 52.7           ~ 45 0
56 Fermi bn130610133 gB 14 57 40.91 +28 12 25.8           ~ 89 0
57 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 180 0
58 Fermi bn090813174 gB 15 00 15.60 +88 34 15.8           ~ 62 0
59 Fermi bn140623224 gB 15 01 53.41 +81 11 29.0           ~ 34 0
60 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 1012 1
61 GRB 060904 gB 15 50.9 +44 59           ~ 10 0
62 GRB 140508A gB 17 01 51.95 +46 46 49.5           ~ 76 0
63 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
64 Fermi bn100413732 gB 17 44 53.22 +15 50 02.4           ~ 62 0
65 GRB 090418A gB 17 57 15.17 +33 24 21.1           ~ 101 0
66 Fermi bn120326056 gB 18 15 37.06 +69 15 35.4           ~ 188 0
67 Fermi bn140506880 gB 18 27 06.04 -55 38 08.7           ~ 113 0
68 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
69 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
70 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
71 Fermi bn140713780 gB 18 44 25.13 +59 38 00.8           ~ 40 0
72 Fermi bn140620219 gB 18 47 29.00 +49 43 51.0           ~ 37 0
73 GRB 080413A gB 19 09 11.73 -27 40 39.6           ~ 163 0
74 Fermi bn140512814 gB 19 17 28.81 -15 05 39.5           ~ 133 0
75 Fermi bn141005217 gB 19 24 22.38 +36 05 42.1           ~ 30 0
76 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
77 GRB 020813A gB 19 46 41.874 -19 36 04.81           ~ 316 0
78 GRB 060105 gB 19 50 00.680 +46 20 55.40           ~ 87 0
79 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
80 GRB 080413B gB 21 44 34.62 -19 58 51.2           ~ 191 0
81 GRB 060117 gB 21 51 36.130 -59 58 39.10           ~ 63 0
82 iPTF 14bfu SN* 21 52 30.00 +32 00 52.5           SNIc 80 0
83 Fermi bn080804972 gB 21 54 41.90 -53 11 20.2           ~ 158 0
84 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
85 GRB 990712 gB 22 31 53.061 -73 24 28.58           ~ 268 1
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 090812 gB 23 32 48.5 -10 36 17           ~ 165 0
89 Fermi bn080810549 gB 23 47 08.00 +00 18 35.1           ~ 240 0
90 GRB 130701A gB 23 48 55.05 +36 06 01.2           ~ 81 0
91 SN 2013fu SN* 23 54 29.91 +29 25 47.6           SNIb/c 144 1

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