CDS

2008A&A...491..157P

Query : 2008A&A...491..157P

2008A&A...491..157P - Astronomy and Astrophysics, volume 491, 157-171 (2008/11-3)

Intrinsic properties of a complete sample of HETE-2 gamma-ray bursts. A measure of the GRB rate in the Local Universe.

PELANGEON A., ATTEIA J.-L., NAKAGAWA Y.E., HURLEY K., YOSHIDA A., VANDERSPEK R., SUZUKI M., KAWAI N., PIZZICHINI G., BOEER M., BRAGA J., CREW G., DONAGHY T.Q., DEZALAY J.P., DOTY J., FENIMORE E.E., GALASSI M., GRAZIANI C., JERNIGAN J.G., LAMB D.Q., LEVINE A., MANCHANDA J., MARTEL F., MATSUOKA M., OLIVE J.-F., PRIGOZHIN G., RICKER G.R., SAKAMOTO T., SHIRASAKI Y., SUGITA S., TAKAGISHI K., TAMAGAWA T., VILLASENOR J., WOOSLEY S.E. and YAMAUCHI M.

Abstract (from CDS):

As a result of the numerous missions dedicated to the detection of Gamma-ray bursts (GRBs), the observed properties of these events are now well known. However, studying their parameters in the source frame is not simple since it requires having measurements of both the bursts' parameters and of their distances. Taking advantage of the forthcoming Catalog of the High Energy Transient Explorer 2 (HETE-2) mission, the aim of this paper is to evaluate the main properties of HETE-2 GRBs - the peak energy (Epeak), the duration (T90) and the isotropic energy (Eiso) - in their source frames and to derive their unbiased distribution. We first construct a complete sample containing all the bursts localized by the Wide-Field X-ray Monitor (WXM) on-board HETE-2, which are selected with a uniform criterion and whose observed parameters can be constrained. We then derive the intrinsic Epeak, T90 and Eiso distributions using their redshift when it is available, or their pseudo-redshift otherwise. We finally compute the ``volume of detectability'' Vmax of each GRB, i.e. the volume of the universe in which the burst is bright enough to be part of our sample, and the corresponding number of GRB within their visibility volume NVmax, in order to derive a weight for each detected burst accounting both for the detection significance and the star formation history of the universe. We obtain unbiased distributions of three intrinsic properties of HETE-2 GRBs: Epeakintr, T90intr and the isotropic energy of the burst. These distributions clearly show the predominence of X-ray flashes (XRFs) in the global GRB population. We also derive the rate of local GRBs: R0H2>11Gpc–3yr–1, which is intermediate between the local rate obtained by considering only the ``high-luminosity'' bursts (∼1Gpc–3yr–1) and that obtained by including the ``low-luminosity'' bursts (>200Gpc–3yr–1). This study shows that the XRFs are predominent in the GRB population and are closely linked to the ``classical'' GRBs. We show that HETE-2 detected no low-luminosity GRB like GRB 980425 or XRF 060218, due to the small size of its detectors, excluding this type of burst from our statistical analysis. The comparison of the GRB rate derived in this study with the known rate of type Ib/c supernovae clearly shows that the progenitors of SNe Ib/c must have some special characteristics in order to produce a gamma-ray burst or an X-ray flash.

Abstract Copyright: ∼

Journal keyword(s): gamma rays: bursts - X-rays: bursts

CDS comments: Paragraph. 3.3 GRB 030531 is GRB 030528 in Simbad.

Simbad objects: 101

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Number of rows : 101
N Identifier Otype ICRS (J2000)
RA 		ICRS (J2000)
DEC 		Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023 		#notes
1 GRB 030824 gB 00 05 02 +19 55.6           ~ 23 0
2 GRB 021016 gB 00 11 04 +49 08.3           ~ 16 0
3 GRB 021021 gB 00 17 23 -01 37.0           ~ 6 0
4 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 537 0
5 GRB 011019 gB 00 42.8 -12 27           ~ 19 0
6 GRB 041006 gB 00 54 50.17 +01 14 07.0           ~ 193 2
7 GRB 021113 gB 01 33 54 +40 27.7           ~ 20 0
8 GRB 041016 gB 01 45 24 -04 39.5           ~ 15 0
9 GRB 051028 gB 01 48 15.010 +47 45 09.20           ~ 37 0
10 GRB 051021A gB 01 56 36.370 +09 04 03.27           ~ 44 0
11 GRB 040924 gB 02 06 22.52 +16 08 48.8           ~ 158 1
12 GRB 021112 gB 02 36 52 +48 50.9           ~ 22 0
13 GRB 011130 gB 03 05 26.9 +03 49 30           ~ 44 0
14 GRB 031026 gB 03 18.7 +28 22           ~ 21 0
15 GRB 011103 gB 03 20 37 +17 40.0           ~ 4 0
16 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 912 1
17 GRB 060115 gB 03 36 08.400 +17 20 43.00           ~ 163 0
18 GRB 021104 gB 03 53 48 +37 57.2           ~ 20 0
19 GRB 031220 gB 04 39.6 +07 22           ~ 22 0
20 GRB 031111 gB 04 47 03.0 +18 06 00           ~ 22 0
21 GRB 011212 gB 05 00 05 +32 07.6           ~ 21 0
22 GRB 041127 gB 05 58 57 +22 43.9           ~ 3 0
23 GRB 041211 gB 06 43 12.0 +20 23 42           ~ 18 0
24 GRB 051211 gB 06 56 13.0 +32 40 44           ~ 15 0
25 GRB 070125 gB 07 51 17.80 +31 09 04.8           ~ 174 0
26 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 531 0
27 SN 2002lt SN* 08 08 59.858 +06 43 37.52           SNIc: 347 1
28 GRB 020127 gB 08 15 05.8 +36 44 31           ~ 64 0
29 GRB 050209 gB 08 26.0 +19 41           ~ 14 0
30 GRB 010110 gB 08 50 22 +73 36.7           ~ 2 0
31 GRB 060121 gB 09 09 51.930 +45 39 45.41           ~ 118 1
32 GRB 020124 gB 09 32 50.8 -11 31 11           ~ 149 0
33 GRB 040228 gB 10 12 12.0 -07 19 33           ~ 11 0
34 GRB 020317 gB 10 23 21 +12 44.6           ~ 18 0
35 GRB 050123 gB 10 31.6 -11 34           ~ 10 0
36 GRB 010213 gB 10 31 36.0 +05 30 39           ~ 23 0
37 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1189 1
38 GRB 030418 gB 10 54 33.69 -07 01 40.8           ~ 67 0
39 GRB 030323 gB 11 06 09.4 -21 46 13           ~ 131 1
40 GRB 030416 gB 11 06 51 -02 53.0           ~ 14 0
41 GRB 030115 gB 11 18 32.6 +15 02 59           ~ 87 1
42 GRB 030226 gB 11 33 04.9 +25 53 56           ~ 198 0
43 GRB 010326 gB 11 57 08 +30 50.5           ~ 15 0
44 GRB 050408 gB 12 02 17.320 +10 51 10.00           ~ 148 0
45 GRB 030328 gB 12 10 48.4 -09 20 51           ~ 142 0
46 GRB 030429 gB 12 13 07.495 -20 54 49.54     23.70     ~ 127 0
47 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 271 1
48 GRB 020305 gB 12 42 27.9 -14 18 12           ~ 41 0
49 GRB 010612 gB 13 02 49 -20 10.6           ~ 8 0
50 GRB 010613 gB 13 02 53 -21 11.0           ~ 10 0
51 GRB 020331 gB 13 16 09.5 -17 55 16           ~ 40 0
52 GRB 030324 gB 13 37 04.4 -00 15 34           ~ 36 0
53 GRB 040511 gB 14 47.8 -44 15           ~ 20 0
54 GRB 030519A gB 14 58 18 -32 57.0           ~ 13 1
55 GRB 020531 gB 15 14 55.8 -19 24 54           ~ 60 0
56 GRB 040425 gB 15 31.6 -39 43           ~ 7 0
57 GRB 010629 gB 16 32 38.3 -18 43 24           ~ 17 1
58 GRB 080210 gB 16 45 04.03 +13 49 36.3           ~ 107 0
59 GRB 030528 gB 17 04 00.3 -22 37 10           ~ 87 1
60 GRB 050922 gB 18 04 23 -32 02.5           ~ 15 0
61 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 370 1
62 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1778 2
63 GRB 020813A gB 19 46 41.874 -19 36 04.81           ~ 299 0
64 GRB 050807 gB 20 13 27 -36 57.0           ~ 6 0
65 GRB 030725 gB 20 33 47 -50 45.8           ~ 26 0
66 GRB 020812 gB 20 38 51 -05 31.2           ~ 26 0
67 GRB 050509 gB 20 42 19.86 +54 04 16.3           ~ 14 0
68 GRB 020625 gB 20 44 14 +07 10.2           ~ 14 0
69 GRB 040701 G 20 47 46.3 -40 14 13           ~ 44 1
70 GRB 040709 gB 20 53.9 -28 13           ~ 4 0
71 GRB 030913 gB 20 58 02 -02 12.5           ~ 22 0
72 GRB 020801 gB 21 02 14 -53 46.2           ~ 15 0
73 GRB 060614 gB 21 23 32.140 -53 01 36.10 18.89 20.12 19.54     ~ 569 1
74 GRB 030823 gB 21 30 47 +21 59.8           ~ 18 0
75 GRB 030821 gB 21 42 33 -45 12.2           ~ 10 0
76 GRB 030723 gB 21 49 24.40 -27 42 47.4           ~ 123 0
77 GRB 040802 gB 21 51 21 -14 11.5           ~ 7 0
78 GRB 060505 gB 22 07 03.440 -27 48 51.89           ~ 250 1
79 GRB 040825B gB 22 46.6 -02 24           ~ 14 0
80 GRB 020903 gB 22 48 42.34 -20 46 09.3           ~ 228 1
81 GRB 031109 gB 22 51 36 -09 18.2           ~ 5 0
82 GRB 010921 gB 22 55 59.90 +40 55 52.9           ~ 167 1
83 GRB 040825A gB 22 59.0 -10 56           ~ 14 0
84 GRB 020819 gB 23 00 12 -43 00.7           ~ 126 1
85 GRB 040916 gB 23 00 55.1 -05 38 43           ~ 35 0
86 GRB 050709 gB 23 01 26.960 -38 58 39.50           ~ 289 1
87 GRB 010928 gB 23 28 55 +30 39.2           ~ 7 0
88 GRB 040810 gB 23 54.1 -35 04           ~ 13 0
89 GRB 051022A gB 23 56 04.200 +19 36 32.30           ~ 177 1
90 GRB 040912 gB 23 56 43.0 -00 55 20           ~ 37 0
91 CXOU J235656.4-005839 X 23 56 56.42 -00 58 39.2           ~ 5 0
92 GRB 040423 gB ~ ~           ~ 5 0
93 GRB 041004 gB ~ ~           ~ 2 0
94 GRB 040131 gB ~ ~           ~ 1 0
95 GRB 001226 gB ~ ~           ~ 1 0
96 GRB 031111B gB ~ ~           ~ 6 0
97 GRB 040319 gB ~ ~           ~ 4 0
98 GRB 050729 gB ~ ~           ~ 5 0
99 GRB 020201 gB ~ ~           ~ 2 0
100 GRB 010225 gB ~ ~           ~ 5 0
101 GRB 030706 gB ~ ~           ~ 6 0

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2023.06.04-18:15:49

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