2011ApJ...735...23N


Query : 2011ApJ...735...23N

2011ApJ...735...23N - Astrophys. J., 735, 23 (2011/July-1)

Heterogeneity in short gamma-ray bursts.

NORRIS J.P., GEHRELS N. and SCARGLE J.D.

Abstract (from CDS):

We analyze the Swift/BAT sample of short gamma-ray bursts, using an objective Bayesian Block procedure to extract temporal descriptors of the bursts' initial pulse complexes (IPCs). The sample is comprised of 12 and 41 bursts with and without extended emission (EE) components, respectively. IPCs of non-EE bursts are dominated by single pulse structures, while EE bursts tend to have two or more pulse structures. The medians of characteristic timescales–durations, pulse structure widths, and peak intervals–for EE bursts are factors of ∼2-3 longer than for non-EE bursts. A trend previously reported by Hakkila and colleagues unifying long and short bursts–the anti-correlation of pulse intensity and width–continues in the two short burst groups, with non-EE bursts extending to more intense, narrower pulses. In addition, we find that preceding and succeeding pulse intensities are anti-correlated with pulse interval. We also examine the short burst X-ray afterglows as observed by the Swift/X-Ray Telescope (XRT). The median flux of the initial XRT detections for EE bursts (∼6x10–10 erg/cm2/s) is ≳ 20x brighter than for non-EE bursts, and the median X-ray afterglow duration for EE bursts (∼60,000 s) is ∼30x longer than for non-EE bursts. The tendency for EE bursts toward longer prompt-emission timescales and higher initial X-ray afterglow fluxes implies larger energy injections powering the afterglows. The longer-lasting X-ray afterglows of EE bursts may suggest that a significant fraction explode into denser environments than non-EE bursts, or that the sometimes-dominant EE component efficiently powers the afterglow. Combined, these results favor different progenitors for EE and non-EE short bursts.

Abstract Copyright:

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

Simbad objects: 64

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Number of rows : 64
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 000218 gB 00 09 44.4 -79 31 49           ~ 4 0
2 GRB 070810B gB 00 35 48.4 +08 49 18           ~ 52 0
3 Fermi bn100117879 gB 00 45 04.56 -01 35 41.7           ~ 137 0
4 GRB 981107 gB 00 49 57.3 +47 29 07           ~ 5 0
5 GRB 050911A gB 00 54 38.290 -38 50 58.50           ~ 63 0
6 GRB 100625A gB 01 03 10.98 -39 05 18.3           ~ 106 0
7 GRB 070724A gB 01 51 14.08 -18 35 38.8           ~ 173 0
8 Fermi bn081024245 gB 01 51 33.80 +61 21 08.2           ~ 68 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 071227A gB 03 52 31.09 -55 59 03.3           ~ 175 0
15 GRB 090815C gB 04 17 57 -65 57.0           ~ 18 0
16 GRB 060313 gB 04 26 28.180 -10 50 37.95 20.55 21.03 19.66     ~ 146 0
17 GRB 061006 gB 07 24 07.660 -79 11 55.10           ~ 192 1
18 GRB 091109B gB 07 30 59.90 -54 05 30.6           ~ 50 0
19 Fermi bn081226044 gB 08 02 00.36 -69 01 46.0           ~ 55 0
20 GRB 051227 gB 08 20 58.107 +31 55 32.01           ~ 121 0
21 GRB 990712A gB 08 24 +07.0           ~ 12 0
22 GRB 090916 gB 08 26 19.60 +25 56 27.3           ~ 27 0
23 GRB 990327 gB 09 32 03.3 -24 53 50           ~ 4 0
24 GRB 061210 gB 09 38 05.270 +15 37 17.30           ~ 134 0
25 GRB 000701B gB 10 01 07.8 -52 07 03           ~ 4 0
26 GRB 090715A gB 10 08 24.50 +10 00 22.4           ~ 23 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 980706 gB 11 00 33 +57 23.1           ~ 21 0
30 GRB 090531A gB 11 54 45.58 +07 44 19.3           ~ 22 0
31 GRB 070923 gB 12 18 29.5 -38 17 38           ~ 36 0
32 GRB 050509B gB 12 36 18.000 +29 01 24.00           ~ 309 1
33 GRB 090426 gB 12 36 19.49 +32 59 05.5           ~ 205 0
34 GRB 090607 gB 12 44 46.70 +44 06 28.4           ~ 37 0
35 GRB 070809 gB 13 35 04.2 -22 07 07           ~ 153 0
36 GRB 060801 gB 14 12 01.290 +16 58 54.00           ~ 157 0
37 GRB 090305 gB 16 07 02.0 -31 34 00           ~ 47 0
38 GRB 050813 gB 16 07 57.190 +11 14 57.80           ~ 138 1
39 GRB 100702A gB 16 22 47.26 -56 31 53.8           ~ 45 0
40 GRB 050724 gB 16 24 44.400 -27 32 27.90     19.70     ~ 438 1
41 GRB 990516 gB 16 29 49.3 +02 43 25           ~ 4 0
42 GRB 071112B gB 17 20 51.0 -80 53 02           ~ 46 0
43 GRB 980605 gB 17 33 36.1 +50 11 54           ~ 4 0
44 GRB 080919 gB 17 40 53.00 -42 22 29.5           ~ 40 0
45 GRB 051105A gB 17 41 10.010 +34 55 45.16 21.26 21.20 20.33     ~ 51 0
46 GRB 060502B gB 18 35 46.060 +52 37 51.45           ~ 140 1
47 GRB 080503 gB 19 06 28.74 +68 47 35.8           ~ 155 0
48 GRB 080905A gB 19 10 39.10 -18 51 55.4           ~ 171 0
49 GRB 050202 gB 19 22 18.0 -38 44 06           ~ 34 0
50 GRB 990313 gB 20 06 57.7 +55 11 27           ~ 4 0
51 GRB 050925 gB 20 13 47.570 +34 19 51.40           ~ 65 0
52 GRB 080702A gB 20 52 12.21 +72 18 46.7           ~ 43 0
53 Fermi bn090621922 gB 20 53 49.30 +69 02 02.9           ~ 59 0
54 GRB 060614 gB 21 23 32.140 -53 01 36.10 18.89 20.12 19.54     ~ 611 1
55 GRB 070429B gB 21 52 03.820 -38 49 42.20           ~ 110 0
56 GRB 070731 gB 21 54 19.5 -15 44 23           ~ 18 0
57 GRB 051221 gB 21 54 48.626 +16 53 27.16 19.49         ~ 351 1
58 GRB 051210 gB 22 00 40.930 -57 36 47.10           ~ 125 0
59 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 187 0
60 GRB 090510 gB 22 14 12.60 -26 35 51.1           ~ 494 1
61 GRB 100213A gB 23 17 34.04 +43 22 44.1           ~ 29 0
62 Fermi bn100816026 gB 23 26 57.56 +26 34 42.6           ~ 149 0
63 GRB 951014A gB ~ ~           ~ 3 0
64 GRB 090715 gB ~ ~           ~ 5 0

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