2012MNRAS.425.1669P


Query : 2012MNRAS.425.1669P

2012MNRAS.425.1669P - Mon. Not. R. Astron. Soc., 425, 1669-1681 (2012/September-3)

The possible ubiquity of energy injection in gamma-ray burst afterglows.

PANAITESCU A. and VESTRAND W.T.

Abstract (from CDS):

Since its launch in 2004, the Swift satellite has monitored the X-ray afterglows of several hundred gamma-ray bursts (GRBs), and revealed that their X-ray light curves are more complex than previously thought, exhibiting up to three power-law segments. Energy injection into the relativistic blast wave energizing the burst ambient medium has been proposed most often to be the reason for the X-ray afterglow complexity. We examine 117 light-curve breaks of 98 Swift X-ray afterglows, selected for their high-quality monitoring and well-constrained flux decay rates. 30 per cent of afterglows have a break that can be an adiabatic jet break, in the sense that there is one variant of the forward-shock emission from a collimated outflow model that can account for both the pre- and post-break flux power-law decay indices, given the measured X-ray spectral slope. If allowance is made for a steady energy injection into the forward shock, then another 56 per cent of X-ray afterglows have a light-curve break that can be explained with a jet break. The remaining 12 per cent that are not jet breaks, as well as the existence of two breaks in 19 afterglows (out of which only one can be a jet break), suggest that some X-ray breaks arise from a sudden change in the rate at which energy is added to the blast wave, and it may well be that a larger fraction of X-ray light-curve breaks are generated by that mechanism. The fractional increase in the shock energy, inferred from the energy injection required to account for the observed X-ray flux decays, may be anticorrelated with the GRB prompt output, whether the X-ray break is a jet break or an energy-injection break. That anticorrelation can also be seen as bursts with a higher energy output being followed by faster fading X-ray afterglows. To test the above two mechanisms for afterglow light-curve breaks, we derive comprehensive analytical results for the dynamics of outflows undergoing energy injection and for their light curves, including closure relations for inverse-Compton afterglows and for the emission from spreading jets interacting with a wind-like ambient medium.

Abstract Copyright: 2012 The Authors Monthly Notices of the Royal Astronomical Society 2012 RAS

Journal keyword(s): radiation mechanisms: non-thermal - relativistic processes - shock waves - gamma-ray burst: general - ISM: jets and outflows

Simbad objects: 98

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Number of rows : 98
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 110420A gB 00 08 39.27 -37 53 11.9           ~ 33 0
2 Fermi bn100522157 gB 00 27 56.79 +09 24 06.6           ~ 57 0
3 GRB 080710 gB 00 33 05.68 +19 30 05.8           ~ 136 0
4 Fermi bn081221681 gB 01 03 10.2 -24 32 53           ~ 186 0
5 Fermi bn100814160 gB 01 29 53.61 -17 59 43.6           ~ 219 0
6 GRB 081222 gB 01 30 57.76 -34 05 44.0           ~ 199 0
7 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
8 Fermi bn091208410 gB 01 57 38.50 +16 52 50.7           ~ 220 0
9 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
10 GRB 091018 gB 02 08 46 -57 33.0           ~ 169 0
11 GRB 070220 gB 02 19 06.810 +68 48 16.11           ~ 57 0
12 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
13 GRB 070129 gB 02 28 00.940 +11 41 04.00       21.3   ~ 120 0
14 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
15 GRB 050822 gB 03 24 27.240 -46 01 59.20     20.82     ~ 115 0
16 GRB 060115 gB 03 36 08.400 +17 20 43.00           ~ 179 0
17 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 275 0
18 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 168 0
19 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 127 0
20 GRB 070328 gB 04 20 27.680 -34 04 00.60 20.29         ~ 97 0
21 Fermi bn101024486 gB 04 26 01.24 -77 15 55.1           ~ 54 0
22 GRB 090407 gB 04 35 54.98 -12 40 45.5           ~ 87 0
23 GRB 100508A gB 05 04 58.99 -20 42 14.1           ~ 39 0
24 GRB 050712 gB 05 10 48.100 +64 54 47.60 19.09   17.86     ~ 71 0
25 GRB 080328A gB 05 21 55.81 +47 30 38.0           ~ 53 0
26 Fermi bn100619015 gB 05 38 28.0 -27 00 02           ~ 57 0
27 Fermi bn100728095 gB 05 55 02.00 -15 15 20.2           ~ 157 0
28 GRB 090401B gB 06 20 21.11 -08 58 20.2           ~ 58 0
29 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
30 GRB 060510 gB 06 23.4 -01 10           ~ 10 0
31 GRB 080703A gB 06 47 12.43 -63 13 08.3           ~ 33 0
32 GRB 060813 gB 07 27 35.380 -29 50 49.40           ~ 62 0
33 GRB 110422A gB 07 28 11.21 +75 06 24.0           ~ 113 0
34 GRB 070628 gB 07 41 06.06 -20 16 45.3           ~ 41 0
35 GRB 071020 gB 07 58 39.65 +32 51 38.8           ~ 158 0
36 GRB 070420 gB 08 04 55.170 -45 33 19.99 20.39 20.01 17.16     ~ 83 0
37 GRB 081028 gB 08 07 34.40 +02 18 16.8           ~ 125 0
38 GRB 060428 gB 08 14.1 -37 10           ~ 5 0
39 GRB 051016B gB 08 48 27.810 +13 39 20.00 20.45         ~ 153 0
40 GRB 110503A gB 08 51 06.31 +52 12 27.7           ~ 115 0
41 Fermi bn100704149 gB 08 54 33.92 -24 12 09.7           ~ 103 0
42 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
43 GRB 061021 gB 09 40 36.120 -21 57 05.40 18.21 19.20 16.82     ~ 160 0
44 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
45 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
46 Fermi bn111228657 gB 10 00 16.04 +18 17 52.2           ~ 201 0
47 GRB 110223B gB 10 00 55.86 -68 18 05.7           ~ 22 0
48 GRB 070107 gB 10 37 36.350 -53 12 47.51 18.37 18.49 17.44     ~ 51 0
49 GRB 110709B gB 10 58 37.2 -23 27 18           ~ 92 0
50 GRB 080430 gB 11 01 14.63 +51 41 07.8           ~ 157 0
51 GRB 101117B gB 11 32 00.54 -72 39 45.9           ~ 27 0
52 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
53 GRB 080320 gB 11 50 56.37 +57 09 25.3           ~ 53 0
54 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
55 GRB 100302A gB 13 02 03.66 +74 35 22.5           ~ 83 0
56 GRB 091130B gB 13 32 35.62 +34 05 18.8           ~ 39 0
57 GRB 060204B gB 14 07 14.900 +27 40 36.40           ~ 93 0
58 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
59 GRB 050802 gB 14 37 05.820 +27 47 12.62 16.85 17.38 16.97     ~ 186 0
60 GRB 090205 gB 14 43 40.00 -27 50 51.4           ~ 99 0
61 GRB 060814 gB 14 45 21.480 +20 35 11.80           ~ 241 0
62 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 180 0
63 Fermi bn090813174 gB 15 00 15.60 +88 34 15.8           ~ 62 0
64 GRB 081203A gB 15 32 07.6 +63 31 15           ~ 177 0
65 GRB 110715A gB 15 50 44.090 -46 14 06.53           ~ 120 0
66 Fermi bn110709642 gB 15 55 33.95 +40 55 27.4       21.4   ~ 59 0
67 GRB 090404 gB 15 56 55.80 +35 31 03.4           ~ 79 0
68 Fermi bn110102788 gB 16 23 31.41 +07 36 49.8           ~ 62 0
69 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
70 GRB 080319C gB 17 15 55.48 +55 23 31.7           ~ 174 0
71 GRB 050814 gB 17 36 45.390 +46 20 21.60           ~ 166 0
72 GRB 090418 gB 17 57 15.2 +33 24 22           ~ 27 0
73 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
74 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
75 GRB 070529 gB 18 54 58.230 +20 39 34.00 20.38   17.25     ~ 98 0
76 GRB 060111B gB 19 05 42.480 +70 22 33.60     17.55     ~ 92 1
77 GRB 060413 gB 19 25 07.850 +13 45 29.90           ~ 69 0
78 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
79 GRB 060105 gB 19 50 00.680 +46 20 55.40           ~ 87 0
80 GRB 050315 gB 20 25 54.100 -42 36 02.19           ~ 225 0
81 GRB 050713B gB 20 31 15.570 +60 56 43.70           ~ 72 0
82 GRB 110915A gB 20 43 17.87 -00 43 23.2           ~ 44 0
83 GRB 070508 gB 20 51 11.810 -78 23 04.88     19.62     ~ 144 0
84 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 204 0
85 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
86 GRB 101023A gB 21 11 51.26 -65 23 17.7           ~ 71 0
87 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
88 GRB 080413B gB 21 44 34.62 -19 58 51.2           ~ 191 0
89 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
90 GRB 051109 gB 22 01 11.0 +40 50 15           ~ 34 0
91 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
92 Fermi bn080916406 gB 22 25 09.30 -57 01 33.7           ~ 177 0
93 GRB 060604 gB 22 28 55.010 -10 54 55.80 20.34 20.31       ~ 134 0
94 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1
95 GRB 081029 gB 23 07 06 -68 10.7           ~ 121 0
96 GRB 050803 gB 23 22 37.910 +05 47 09.00           ~ 127 0
97 GRB 061222 gB 23 53.0 +46 32           ~ 18 0
98 GRB 051022A gB 23 56 04.200 +19 36 32.30           ~ 194 1

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