2009ApJ...707..328L


Query : 2009ApJ...707..328L

2009ApJ...707..328L - Astrophys. J., 707, 328-342 (2009/December-2)

A comprehensive analysis of Swift/X-ray telescope data. IV. Single power-law decaying light curves versus canonical light curves and implications for a unified origin of X-rays.

LIANG E.-W., LU H.-J., HOU S.-J., ZHANG B.-B. and ZHANG B.

Abstract (from CDS):

By systematically analyzing the Swift/XRT light curves detected before 2009 July, we find 19 light curves that monotonously decay as a single power law (SPL) with an index of 1 ∼ 1.7 from tens (or hundreds) of seconds to ∼105 s post the gamma-ray burst (GRB) trigger. They are apparently different from the canonical light curves characterized by a shallow-to-normal decay transition. We compare the observations of the prompt gamma rays and the X-rays for these two samples of GRBs (SPL vs. canonical). No statistical difference is found in the prompt gamma-ray properties for the two samples. The X-ray properties of the two samples are also similar, although the SPL sample tends to have a slightly lower neutral hydrogen absorption column for the host galaxies and a slightly larger energy release compared with the canonical sample. The SPL X-ray Telescope (XRT) light curves in the burst frame gradually merge into a conflux, and their luminosities at 105 s are normally distributed at log L/ergs/s = 45.6±0.5. The normal decay segment of the canonical XRT light curves has the same feature. Similar to the normal decay segment, the SPL light curves satisfy the closure relations and therefore can be roughly explained with external shock models. In the scenario that the X-rays are the afterglows of the GRB fireball, our results indicate that the shallow decay would be due to energy injection into the fireball and the total energy budget after injection for both samples of GRBs is comparable. More intriguing, we find that a prior X-ray emission model proposed by Yamazaki is more straightforward to interpret the observed XRT data. We show that the zero times (T0) of the X-rays are 102-105 s prior to the GRB trigger for the canonical sample, and satisfy a log-normal distribution. The negligible T0's of the SPL sample are consistent with being the tail of T0distributions at low end, suggesting that the SPL sample and the canonical sample may be from a same parent sample. Referenced to T0, the canonical XRT light curves well trace the SPL light curves. The T0's of the canonical light curves in our analysis are usually much larger than the offsets of the known precursors from the main GRBs. If the prior emission hypothesis is real, the X-ray emission is better interpreted within the external shock models based on the spectral and temporal indices of the X-rays. The lack of detection of a jet-like break in most XRT light curves implies that the opening angle of the prior emission jet would be usually large.

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Journal keyword(s): gamma rays: bursts - gamma rays: observations - methods: data analysis - radiation mechanisms: non-thermal

Simbad objects: 72

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Number of rows : 72
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 070110 gB 00 03 39.270 -52 58 27.00 21.8 21.9 21.2     ~ 220 0
2 GRB 060912 gB 00 21 08.160 +20 58 17.80 17.61   17.56     ~ 42 0
3 GRB 090123 gB 00 27 10.50 -23 30 12.6           ~ 32 0
4 GRB 080710 gB 00 33 05.68 +19 30 05.8           ~ 136 0
5 GRB 050824 gB 00 48 56.100 +22 36 32.00 19.66 21.03 20.46 23.70   ~ 184 0
6 GRB 081222 gB 01 30 57.76 -34 05 44.0           ~ 199 0
7 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
8 GRB 080707 gB 02 10 28.48 +33 06 35.1           ~ 83 0
9 GRB 060906 gB 02 43 00.900 +30 21 42.12     19.84     ~ 147 0
10 Fermi bn080913735 gB 03 00 -03.0           ~ 18 0
11 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 315 1
12 GRB 070318 gB 03 13 56.830 -42 56 46.30 18.27 16.23 15.49     ~ 170 0
13 GRB 060115 gB 03 36 08.400 +17 20 43.00           ~ 179 0
14 GRB 060124 gB 05 08 25.900 +69 44 26.98   18.91 17.35     ~ 280 0
15 GRB 060116 gB 05 38 46.170 -05 26 15.08           ~ 86 0
16 GRB 090401B gB 06 20 21.11 -08 58 20.2           ~ 58 0
17 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
18 GRB 070411 gB 07 09 19.930 +01 03 52.60     17.94     ~ 138 0
19 GRB 071020 gB 07 58 39.65 +32 51 38.8           ~ 158 0
20 GRB 080516 gB 08 02 34.16 -26 09 35.3           ~ 59 0
21 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
22 GRB 051016B gB 08 48 27.810 +13 39 20.00 20.45         ~ 153 0
23 GRB 080307 gB 09 06 30.73 +35 08 19.8           ~ 53 0
24 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
25 GRB 050505 gB 09 27 03.300 +30 16 23.70     20.74     ~ 206 0
26 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
27 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
28 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
29 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
30 GRB 080430 gB 11 01 14.63 +51 41 07.8           ~ 157 0
31 GRB 011211 gB 11 15 16 -21 56.0           ~ 305 0
32 GRB 011121 gB 11 34 26.67 -76 01 41.6       23.0   ~ 286 1
33 GRB 080714 gB 12 32 25.29 -60 16 40.2           ~ 54 0
34 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
35 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
36 GRB 070810A gB 12 39 51.18 +10 45 02.8           ~ 80 0
37 GRB 060512 gB 13 03 05.810 +41 11 27.21 19.12 19.63 17.20     ~ 142 0
38 GRB 090529 gB 14 09 52.49 +24 27 33.5           ~ 89 0
39 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
40 GRB 050802 gB 14 37 05.820 +27 47 12.62 16.85 17.38 16.97     ~ 186 0
41 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 214 0
42 GRB 060814 gB 14 45 21.480 +20 35 11.80           ~ 241 0
43 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 180 0
44 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
45 GRB 080906 gB 15 12 13 -80 32.4           ~ 63 0
46 GRB 081203A gB 15 32 07.6 +63 31 15           ~ 177 0
47 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
48 GRB 060502A gB 16 03 42.480 +66 36 02.49     18.65     ~ 143 0
49 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
50 GRB 080210 gB 16 45 04.03 +13 49 36.3           ~ 121 0
51 GRB 050721 gB 16 53 44.530 -28 22 51.80     19.63     ~ 62 0
52 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
53 GRB 090418A gB 17 57 15.17 +33 24 21.1           ~ 101 0
54 GRB 070330 gB 17 58 09.980 -63 47 34.80     18.87     ~ 48 0
55 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
56 GRB 070529 gB 18 54 58.230 +20 39 34.00 20.38   17.25     ~ 98 0
57 GRB 060111B gB 19 05 42.480 +70 22 33.60     17.55     ~ 92 1
58 GRB 080413A gB 19 09 11.73 -27 40 39.6           ~ 163 0
59 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
60 Fermi bn080905705 gB 20 06 57.93 -62 33 46.8           ~ 119 0
61 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 181 0
62 GRB 070508 gB 20 51 11.810 -78 23 04.88     19.62     ~ 144 0
63 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
64 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
65 GRB 060522 gB 21 31 44.850 +02 53 10.80           ~ 140 0
66 GRB 080413B gB 21 44 34.62 -19 58 51.2           ~ 191 0
67 Fermi bn080804972 gB 21 54 41.90 -53 11 20.2           ~ 158 0
68 GRB 060927A gB 21 58 11.930 +05 21 50.32           ~ 215 0
69 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
70 GRB 051109A gB 22 01 15.320 +40 49 23.70   20.09 20.14     ~ 190 0
71 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1
72 GRB 071025 gB 23 40 17.02 +31 46 42.4           ~ 122 0

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