2013ApJ...764..179B


Query : 2013ApJ...764..179B

2013ApJ...764..179B - Astrophys. J., 764, 179 (2013/February-3)

Short versus long and collapsars versus non-collapsars: a quantitative classification of gamma-ray bursts.

BROMBERG O., NAKAR E., PIRAN T. and SARI R.

Abstract (from CDS):

Gamma-ray bursts (GRBs) are traditionally divided into long and short according to their durations ({lg}2 s). It was generally believed that this reflects a different physical origin: collapsars (long) and non-collapsars (short). We have recently shown that the duration distribution of collapsars is flat, namely, independent of the duration, at short durations. Using this model for the distribution of Collapsars we determine the duration distribution of non-Collapsars and estimate the probability that a burst with a given duration (and hardness) is a Collapsar or not. We find that this probability depends strongly on the spectral window of the observing detector. While the commonly used limit of 2 s is conservative and suitable for BATSE bursts, 40% of Swift's bursts shorter than 2 s are Collapsars and the division {lg}0.8 s is more suitable for Swift. We find that the duration overlap of the two populations is very large. On the one hand there is a non-negligible fraction of non-Collapsars longer than 10 s, while on the other hand even bursts shorter than 0.5 s in the Swift sample have a non-negligible probability to be Collapsars. Our results enable the construction of non-Collapsar samples while controlling the Collapsar contamination. They also highlight that no firm conclusions can be drawn based on a single burst and they have numerous implications concerning previous studies of non-Collapsar properties that were based on the current significantly contaminated Swift samples of localized short GRBs. Specifically (1) all known short bursts with z > 1 are most likely Collapsars; (2) the only short burst with a clear jet break is most likely a Collapsar, indicating our lack of knowledge concerning non-Collapsar beaming; and (3) the existence of non-Collapsars with durations up to 10 s imposes new challenges to non-Collapsar models.

Abstract Copyright:

Journal keyword(s): gamma-ray burst: general - methods: data analysis

Simbad objects: 65

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Number of rows : 65
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 GRB 070810B gB 00 35 48.4 +08 49 18           ~ 52 0
2 Fermi bn100117879 gB 00 45 04.56 -01 35 41.7           ~ 137 0
3 Fermi bn111117510 gB 00 50 46.220 +23 00 39.22           ~ 120 0
4 GRB 100625A gB 01 03 10.98 -39 05 18.3           ~ 106 0
5 GRB 080426 gB 01 45 59.79 +69 28 06.0           ~ 45 0
6 GRB 070724A gB 01 51 14.08 -18 35 38.8           ~ 173 0
7 Fermi bn081024245 gB 01 51 33.80 +61 21 08.2           ~ 68 0
8 GRB 090417A gB 02 19 59.0 -07 10 51           ~ 34 0
9 GRB 070714A gB 02 51 43.36 +30 14 35.1           ~ 58 0
10 GRB 070209 gB 03 04 51.200 -47 22 34.19           ~ 43 0
11 Fermi bn100206563 gB 03 08 38.94 +13 09 25.5           ~ 126 0
12 GRB 050906 gB 03 31 15.28 -14 36 30.1           ~ 71 1
13 GRB 070729 gB 03 45 16.04 -39 19 19.9           ~ 72 0
14 GRB 070714B gB 03 51 22.30 +28 17 51.3           ~ 216 1
15 GRB 071227A gB 03 52 31.09 -55 59 03.3           ~ 175 0
16 GRB 090815C gB 04 17 57 -65 57.0           ~ 18 0
17 GRB 060313 gB 04 26 28.180 -10 50 37.95 20.55 21.03 19.66     ~ 146 0
18 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 129 0
19 Fermi bn081101491 gB 06 23 20.70 -00 06 41.5           ~ 36 0
20 GRB 061006 gB 07 24 07.660 -79 11 55.10           ~ 193 1
21 GRB 091109B gB 07 30 59.90 -54 05 30.6           ~ 50 0
22 Fermi bn081226044 gB 08 02 00.36 -69 01 46.0           ~ 55 0
23 GRB 080121 gB 09 08 56.0 +41 50 29           ~ 35 0
24 GRB 060121 gB 09 09 51.930 +45 39 45.41           ~ 123 1
25 GRB 061210 gB 09 38 05.270 +15 37 17.30           ~ 134 0
26 Fermi bn101129652 gB 10 23 41 -17 38.7           ~ 33 0
27 GRB 061217 gB 10 41 39.320 -21 07 22.11           ~ 122 0
28 GRB 090515 gB 10 56 41.0 +14 27 22           ~ 107 0
29 GRB 070923 gB 12 18 29.5 -38 17 38           ~ 36 0
30 GRB 050509B gB 12 36 18.000 +29 01 24.00           ~ 309 1
31 GRB 090426 gB 12 36 19.49 +32 59 05.5           ~ 205 0
32 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 161 0
33 GRB 070406 gB 13 15 51.350 +16 30 46.90 20.54         ~ 49 0
34 GRB 070809 gB 13 35 04.2 -22 07 07           ~ 153 0
35 GRB 100424A gB 13 57 47.46 +01 32 20.3           ~ 62 0
36 GRB 060801 gB 14 12 01.290 +16 58 54.00           ~ 157 0
37 GRB 100628A gB 15 03 53.59 -31 39 50.4           ~ 46 0
38 GRB 090305 gB 16 07 02.0 -31 34 00           ~ 47 0
39 GRB 050813 gB 16 07 57.190 +11 14 57.80           ~ 138 1
40 GRB 100702A gB 16 22 47.26 -56 31 53.8           ~ 45 0
41 GRB 050724 gB 16 24 44.400 -27 32 27.90     19.70     ~ 439 1
42 GRB 071112B gB 17 20 51.0 -80 53 02           ~ 46 0
43 GRB 080919 gB 17 40 53.00 -42 22 29.5           ~ 40 0
44 GRB 051105A gB 17 41 10.010 +34 55 45.16 21.26 21.20 20.33     ~ 51 0
45 GRB 070707 gB 17 50 58.49 -68 55 27.0           ~ 60 1
46 GRB 111126A gB 18 24 14 +51 27.7           ~ 14 0
47 GRB 060502B gB 18 35 46.060 +52 37 51.45           ~ 140 1
48 Fermi bn101224227 gB 19 03 41.91 +45 42 48.5           ~ 53 0
49 GRB 111020A gB 19 08 12.53 -38 00 43.0           ~ 59 0
50 GRB 080905A gB 19 10 39.10 -18 51 55.4           ~ 171 0
51 GRB 050202 gB 19 22 18.0 -38 44 06           ~ 34 0
52 GRB 050925 gB 20 13 47.570 +34 19 51.40           ~ 65 0
53 GRB 080702A gB 20 52 12.21 +72 18 46.7           ~ 43 0
54 Fermi bn090621922 gB 20 53 49.30 +69 02 02.9           ~ 59 0
55 Fermi bn110420946 gB 21 20 10.90 -41 16 38.0           ~ 34 0
56 GRB 060614 gB 21 23 32.140 -53 01 36.10 18.89 20.12 19.54     ~ 612 1
57 GRB 070429B gB 21 52 03.820 -38 49 42.20           ~ 110 0
58 GRB 051221 gB 21 54 48.626 +16 53 27.16 19.49         ~ 351 1
59 GRB 110112A gB 21 59 43.77 +26 27 24.4           ~ 40 0
60 GRB 051210 gB 22 00 40.930 -57 36 47.10           ~ 125 0
61 GRB 060505 gB 22 07 03.440 -27 48 51.89           ~ 259 1
62 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 187 0
63 GRB 090510 gB 22 14 12.60 -26 35 51.1           ~ 494 1
64 GRB 080123 gB 22 35 46.100 -64 54 03.24           ~ 88 0
65 GRB 050709 gB 23 01 26.960 -38 58 39.50           ~ 297 1

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