2012A&A...538A.134X


Query : 2012A&A...538A.134X

2012A&A...538A.134X - Astronomy and Astrophysics, volume 538A134-134 (2012/2-1)

New three-parameter correlation for gamma-ray bursts with a plateau phase in the afterglow.

XU M. and HUANG Y.F.

Abstract (from CDS):

Gamma ray bursts (GRBs) offer strong advantages because of their huge burst energies, luminosities, and high redshifts in probing the Universe. A few interesting luminosity correlations of GRBs have been used to test cosmology models. Especially, for a subsample of long GRBs with known redshifts and a plateau phase in the afterglow, a correlation between the end time of the plateau phase (in the GRB rest frame) and the corresponding X-ray luminosity has been found. Here, we add the isotropic γ-ray energy release as a third parameter to get a tighter three-parameter correlation. We reanalyzed the subsample and found that a significantly tighter correlation exists when we add the isotropic γ-ray energy release into the consideration. We used the Markov-chain Monte Carlo techniques to get the best-fit coefficients. A new three-parameter correlation is found for the GRBs with an obvious plateau phase in the afterglow. The best fit correlation is found to be LX ∝Ta–0.87Eγ,iso0.88. Additionally, both long and intermediate duration GRBs are consistent with the same three-parameter correlation equation. We argue that the new three-parameter correlation is consistent with the hypothesis that the subsample of GRBs with a plateau phase in the afterglow is associated with the birth of rapidly rotating magnetars and that the plateau is due to the continuous energy-injection from the magnetar. It is suggested that the newly born millisecond magnetars associated with GRBs might provide a good standard candle in the Universe.

Abstract Copyright: ∼

Journal keyword(s): ISM: jets and outflows - gamma-ray burst: general

Simbad objects: 69

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Number of rows : 69
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 060912A gB 00 21 08.11 +20 58 18.9           ~ 116 1
3 GRB 071031 gB 00 25 37.40 -58 03 33.9           ~ 184 0
4 GRB 050824 gB 00 48 56.100 +22 36 32.00 19.66 21.03 20.46 23.70   ~ 184 0
5 GRB 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
6 GRB 050908 gB 01 21 50.750 -12 57 17.20           ~ 179 0
7 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
8 GRB 070721B gB 02 12 32.98 -02 11 39.8           ~ 128 0
9 GRB 060202 gB 02 23 22.940 +38 23 03.70           ~ 102 0
10 GRB 070802 gB 02 27 35.91 -55 31 39.1           ~ 168 0
11 GRB 050603 gB 02 39 56.839 -25 10 54.92     18.48     ~ 174 0
12 GRB 060906 gB 02 43 00.900 +30 21 42.12     19.84     ~ 147 0
13 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 315 1
14 GRB 050318 gB 03 18 51.000 -46 23 43.61 18.10 18.68 17.58     ~ 189 0
15 GRB 060115 gB 03 36 08.400 +17 20 43.00           ~ 179 0
16 GRB 060223A gB 03 40 49.560 -17 07 48.40     17.90     ~ 98 0
17 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
18 GRB 060124 gB 05 08 25.900 +69 44 26.98   18.91 17.35     ~ 280 0
19 GRB 060116 gB 05 38 46.170 -05 26 15.08           ~ 86 0
20 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
21 GRB 071020 gB 07 58 39.65 +32 51 38.8           ~ 158 0
22 GRB 051016B gB 08 48 27.810 +13 39 20.00 20.45         ~ 153 0
23 GRB 050505 gB 09 27 03.300 +30 16 23.70     20.74     ~ 206 0
24 GRB 060108 gB 09 48 01.980 +31 55 08.59           ~ 107 0
25 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
26 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
27 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
28 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
29 GRB 080430 gB 11 01 14.63 +51 41 07.8           ~ 157 0
30 GRB 080603B gB 11 46 07.46 +68 03 38.5           ~ 153 0
31 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
32 GRB 070810A gB 12 39 51.18 +10 45 02.8           ~ 80 0
33 GRB 060512 gB 13 03 05.810 +41 11 27.21 19.12 19.63 17.20     ~ 142 0
34 GRB 070208 gB 13 11 32.607 +61 57 54.37 20.79 20.79 19.86     ~ 119 0
35 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
36 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
37 GRB 050801 gB 13 36 35.000 -21 55 41.00 15.03 15.82 15.46     ~ 164 0
38 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 327 0
39 GRB 050802 gB 14 37 05.820 +27 47 12.62 16.85 17.38 16.97     ~ 186 0
40 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 214 0
41 GRB 060814 gB 14 45 21.480 +20 35 11.80           ~ 241 0
42 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
43 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
44 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
45 GRB 060904 gB 15 50.9 +44 59           ~ 10 0
46 GRB 060510B gB 15 56 29.200 +78 34 12.00           ~ 155 0
47 GRB 060502A gB 16 03 42.480 +66 36 02.49     18.65     ~ 143 0
48 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
49 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
50 GRB 070518 gB 16 56 47.750 +55 17 41.40 18.68 19.22 19.01     ~ 75 0
51 GRB 050814 gB 17 36 45.390 +46 20 21.60           ~ 166 0
52 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
53 GRB 070529 gB 18 54 58.230 +20 39 34.00 20.38   17.25     ~ 98 0
54 GRB 050315 gB 20 25 54.100 -42 36 02.19           ~ 225 0
55 GRB 070508 gB 20 51 11.810 -78 23 04.88     19.62     ~ 144 0
56 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
57 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
58 GRB 060605 gB 21 28 37.320 -06 03 31.30   20.12 16.53     ~ 210 0
59 GRB 060522 gB 21 31 44.850 +02 53 10.80           ~ 140 0
60 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
61 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
62 GRB 051109A gB 22 01 15.320 +40 49 23.70   20.09 20.14     ~ 190 0
63 GRB 060604 gB 22 28 55.010 -10 54 55.80 20.34 20.31       ~ 134 0
64 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
65 GRB 051109B gB 23 01 50.330 +38 40 46.51           ~ 93 0
66 GRB 070506 gB 23 08 52.390 +10 43 20.30     19.04     ~ 86 0
67 GRB 050803 gB 23 22 37.910 +05 47 09.00           ~ 127 0
68 Fermi bn080810549 gB 23 47 08.00 +00 18 35.1           ~ 240 0
69 GRB 060707 gB 23 48 19.000 -17 54 17.00     19.79     ~ 170 0

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