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 - 2026
#notes
1 GRB 070810B gB 00 35 48.4 +08 49 18           ~ 57 0
2 Fermi bn100117879 G 00 45 04.6610 -01 35 42.020           ~ 155 0
3 Fermi bn111117510 gB 00 50 46.220 +23 00 39.22           ~ 141 0
4 GRB 100625A gB 01 03 10.98 -39 05 18.3           ~ 124 0
5 GRB 080426 gB 01 45 59.79 +69 28 06.0           ~ 50 0
6 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
7 Fermi bn081024245 gB 01 51 33.80 +61 21 08.2           ~ 75 0
8 GRB 090417A gB 02 19 59.0 -07 10 51           ~ 36 0
9 GRB 070714A gB 02 51 43.36 +30 14 35.1           ~ 63 0
10 GRB 070209 gB 03 04 51.200 -47 22 34.19           ~ 45 0
11 PSO J047.1631+13.1580 G 03 08 39.14930640 +13 09 29.0253240           ~ 144 0
12 GRB 050906 gB 03 31 15.28 -14 36 30.1           ~ 76 1
13 GRB 070729 gB 03 45 16.04 -39 19 19.9           ~ 81 0
14 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
15 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
16 GRB 090815C gB 04 17 57 -65 57.0           ~ 19 0
17 GRB 060313 G 04 26 28.4020 -10 50 39.901 20.55 21.03 19.66     ~ 156 0
18 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
19 Fermi bn081101491 gB 06 23 20.70 -00 06 41.5           ~ 39 0
20 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
21 GRB 091109B gB 07 30 59.90 -54 05 30.6           ~ 57 0
22 Fermi bn081226044 G 08 02 00.4500 -69 01 49.500           ~ 63 0
23 GRB 080121 gB 09 08 56.0 +41 50 29           ~ 40 0
24 NAME GRB 060121 HOST Galaxy G 09 09 52.0260 +45 39 45.538       26.6   ~ 127 0
25 SDSS J093805.33+153719.0 G 09 38 05.33384 +15 37 19.0406           ~ 146 0
26 Fermi bn101129652 gB 10 23 41 -17 38.7           ~ 34 0
27 GRB 061217 gB 10 41 39.320 -21 07 22.11           ~ 128 0
28 GRB 090515 gB 10 56 41.0 +14 27 22           ~ 122 0
29 GRB 070923 gB 12 18 29.5 -38 17 38           ~ 38 0
30 SDSS J123612.87+285858.8 BiC 12 36 12.8803407000 +28 58 58.780075656           ~ 328 1
31 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
32 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 198 0
33 GRB 070406 gB 13 15 51.350 +16 30 46.90 20.54         ~ 50 0
34 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
35 GRB 100424A gB 13 57 47.46 +01 32 20.3           ~ 71 0
36 GRB 060801 G 14 12 01.2620 +16 58 55.970           ~ 172 0
37 GRB 100628A gB 15 03 53.59 -31 39 50.4           ~ 50 0
38 GRB 090305 G 16 07 07.5960 -31 33 22.540           ~ 53 0
39 GRB 050813 gB 16 07 57.190 +11 14 57.80           ~ 147 0
40 GRB 100702A gB 16 22 47.26 -56 31 53.8           ~ 53 0
41 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
42 GRB 071112B gB 17 20 51.0 -80 53 02           ~ 50 0
43 GRB 080919 gB 17 40 53.00 -42 22 29.5           ~ 49 0
44 GRB 051105A gB 17 41 10.010 +34 55 45.16 21.26 21.20 20.33     ~ 53 0
45 NAME GRB 070707 HOST Galaxy G 17 50 58.5550 -68 55 27.600       27.3   ~ 63 0
46 GRB 111126A gB 18 24 14 +51 27.7           ~ 14 0
47 GRB 060502B gB 18 35 46.060 +52 37 51.45           ~ 153 1
48 PSO J285.9246+45.7134 G 19 03 41.90914320 +45 42 48.4220520           ~ 63 0
49 GRB 111020A gB 19 08 12.53 -38 00 43.0           ~ 66 0
50 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
51 GRB 050202 gB 19 22 18.0 -38 44 06           ~ 36 0
52 GRB 050925 gB 20 13 47.570 +34 19 51.40           ~ 72 0
53 GRB 080702A gB 20 52 12.21 +72 18 46.7           ~ 47 0
54 Fermi bn090621922 gB 20 53 49.30 +69 02 02.9           ~ 65 0
55 Fermi bn110420946 gB 21 20 10.90 -41 16 38.0           ~ 39 0
56 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
57 GRB 070429B G 21 52 03.6910 -38 49 42.820           ~ 125 0
58 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
59 GRB 110112A gB 21 59 43.77 +26 27 24.4           ~ 47 0
60 GRB 051210 gB 22 00 40.930 -57 36 47.10           ~ 138 0
61 GRB 060505 gB 22 07 03.440 -27 48 51.89           ~ 286 1
62 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
63 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
64 GRB 080123 gB 22 35 46.100 -64 54 03.24           ~ 98 0
65 NVSS J230126-385839 rG 23 01 26.7650 -38 58 40.422   22.22 21.22 21   ~ 325 1

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