2006ApJ...646..351L


Query : 2006ApJ...646..351L

2006ApJ...646..351L - Astrophys. J., 646, 351-357 (2006/July-3)

Testing the curvature effect and internal origin of gamma-ray burst prompt emissions and X-ray flares with Swift data.

LIANG E.W., ZHANG B., O'BRIEN P.T., WILLINGALE R., ANGELINI L., BURROWS D.N., CAMPANA S., CHINCARINI G., FALCONE A., GEHRELS N., GOAD M.R., GRUPE D., KOBAYASHI S., MESZAROS P., NOUSEK J.A., OSBORNE J.P., PAGE K.L. and TAGLIAFERRI G.

Abstract (from CDS):

The X-ray light curves of many GRBs have a steep tail following the gamma-rays and have some erratic flares. We assume that these tails and flares are of ``internal'' origin and that their decline behaviors are dominated by the curvature effect. This effect suggests that the decay slope of the late steep decay part of the light curves is α=2+β, where β is the X-ray spectral index. We present a self-consistency test for this scenario with a sample of 36 prompt emission tails/flares in 22 light curves observed by the Swift XRT. We derive the zero time (t0) for each steep decay component by fitting the light curves with the constraint of α=2+β. Our results show that the t0 values of the prompt emission tails and the tails of well-separated flares are self-consistent with the expectation of the internal dissipation models, indicating that each X-ray flare forms a distinct episode of the central engine activity and the central engine remains active after the prompt emission is over, sometimes up to ∼1 day after the GRB trigger. This challenges the conventional models and calls for new ideas to restart the central engine. We further show that the onset time of the late central engine activity does not depend on the GRB duration. We also identify a minority group of GRBs whose combined BAT-XRT light curves are smoothly connected, without an abrupt transition between the prompt emission and the afterglow. These GRBs may have an external origin for both the prompt emission and the afterglow.

Abstract Copyright: ∼

Journal keyword(s): Gamma Rays: Bursts - Methods: Statistical

Simbad objects: 26

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Number of rows : 26
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 050406 gB 02 17 52.200 -50 11 15.81     18.83     ~ 125 0
2 GRB 050822 gB 03 24 27.240 -46 01 59.20     20.82     ~ 115 0
3 GRB 050712 gB 05 10 48.100 +64 54 47.60 19.09   17.86     ~ 71 0
4 GRB 050826 gB 05 51 01.590 -02 38 35.40           ~ 136 0
5 GRB 050502B gB 09 30 10.024 +16 59 48.07           ~ 169 0
6 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
7 GRB 050219A gB 11 05 38.990 -40 41 03.00           ~ 97 0
8 GRB 050714B gB 11 18 47.610 -15 32 48.90           ~ 80 0
9 GRB 050801 gB 13 36 35.000 -21 55 41.00 15.03 15.82 15.46     ~ 164 0
10 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 327 0
11 GRB 050717 gB 14 17 24.440 -50 32 00.10           ~ 68 0
12 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
13 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
14 GRB 050721 gB 16 53 44.530 -28 22 51.80     19.63     ~ 62 0
15 GRB 050814 gB 17 36 45.390 +46 20 21.60           ~ 166 0
16 GRB 050126 gB 18 32 27.22 +42 22 14.2           ~ 129 0
17 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
18 GRB 050607 gB 20 00 42.790 +09 08 31.50   19.55 18.94     ~ 103 0
19 GRB 050315 gB 20 25 54.100 -42 36 02.19           ~ 225 0
20 GRB 050421 gB 20 29 02.850 +73 39 17.91           ~ 75 0
21 GRB 050713B gB 20 31 15.570 +60 56 43.70           ~ 72 0
22 GRB 050713A gB 21 22 09.530 +77 04 29.50           ~ 125 0
23 GRB 050422 gB 21 37 54.650 +55 46 46.40     19.85     ~ 45 0
24 GRB 050716 gB 22 34 20.730 +38 41 03.60   21.52 20.32     ~ 76 0
25 GRB 050803 gB 23 22 37.910 +05 47 09.00           ~ 127 0
26 GRB 050819 gB 23 55 01.650 +24 51 38.80           ~ 75 0

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