2021ApJ...920..135X

Query : 2021ApJ...920..135X

2021ApJ...920..135X - Astrophys. J., 920, 135-135 (2021/October-3)

X-ray plateaus in gamma-ray burst afterglows and their application in cosmology.

XU F., TANG C.-H., GENG J.-J., WANG F.-Y., WANG Y.-Y., KUERBAN A. and HUANG Y.-F.

Abstract (from CDS):

For gamma-ray bursts (GRBs) with a plateau phase in the X-ray afterglow, a so-called L-T-E correlation that tightly connects the isotropic energy of the prompt GRB (Eγ,iso) with the end time of the X-ray plateau (Ta) and the corresponding X-ray luminosity at the end time (LX) has been found. Here we show that there is a clear redshift evolution in the correlation. Furthermore, because the power-law indices of LX and Eγ,iso in the correlation function are almost identical, the L-T-E correlation is insensitive to cosmological parameters and cannot be used as a satisfactory standard candle. On the other hand, based on a sample including 121 long GRBs, we establish a new three-parameter correlation that connects LX, Ta, and the spectral peak energy Ep, i.e., the L-T-Ep correlation. This correlation strongly supports the so-called Combo-relation established by Izzo et al. After correcting for the redshift evolution, we show that the de-evolved L-T-Ep correlation can be used as a standard candle. By using this correlation alone, we are able to constrain the cosmological parameters as Ωm=0.389–0.141+0.202 (1σ) for the flat ΛCDM model, or Ωm=0.369–0.191+0.217 and w=-0.966–0.678+0.513 (1σ) for the flat wCDM model. Combining with other cosmological probes, more accurate constraints on the cosmology models are presented.

Abstract Copyright: © 2021. The American Astronomical Society. All rights reserved.

Journal keyword(s): Cosmology - Cosmological parameters - Dark energy - Dark matter - Gamma-ray bursts - Neutron stars

Simbad objects: 121

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Number of rows : 121
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 180720B gB 00 02 06.99 -02 55 07.8           ~ 215 0
2 GRB 170607A gB 00 29 27.84 +09 14 35.5           ~ 62 0
3 GRB 060708 gB 00 31 13.850 -33 45 32.40 19.07 19.79 17.37     ~ 109 0
4 SN 2010ma SN* 00 48 55.35 -34 33 59.5           SNIc 190 1
5 Fermi bn140703026 gB 00 51 58.99 +45 06 05.4           ~ 90 0
6 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
7 Fermi bn081221681 gB 01 03 10.2 -24 32 53           ~ 186 0
8 Fermi bn100814160 gB 01 29 53.61 -17 59 43.6           ~ 219 0
9 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
10 Fermi bn091208410 gB 01 57 38.50 +16 52 50.7           ~ 220 0
11 Fermi bn140304557 gB 02 02 33.90 +33 28 27.9           ~ 106 0
12 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
13 Fermi bn090113778 gB 02 08 16.00 +33 26 08.4           ~ 92 0
14 GRB 091018 gB 02 08 46 -57 33.0           ~ 169 0
15 GRB 170714A gB 02 17 17 +01 58.0           ~ 50 0
16 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
17 GRB 070129 gB 02 28 00.940 +11 41 04.00       21.3   ~ 120 0
18 GRB 060906 gB 02 43 00.900 +30 21 42.12     19.84     ~ 147 0
19 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
20 GRB 120802A gB 02 59 22.04 +13 46 05.0           ~ 76 0
21 GRB 100902A gB 03 14 30 +30 58.2           ~ 68 0
22 GRB 060115 gB 03 36 08.400 +17 20 43.00           ~ 179 0
23 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 275 0
24 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
25 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 168 0
26 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 127 0
27 Fermi bn170113420 gB 04 06 59 -71 56.0           ~ 64 0
28 GRB 090407 gB 04 35 54.98 -12 40 45.5           ~ 87 0
29 Fermi bn131105087 gB 04 43 53.50 -63 00 17.7           ~ 95 0
30 GRB 151027B gB 05 04 52.67 -06 27 00.7           ~ 61 0
31 GRB 111229A gB 05 05 08.86 -84 42 39.1           ~ 47 0
32 Fermi bn141004973 gB 05 06 56.11 +12 49 10.1           ~ 75 0
33 GRB 180329B gB 05 31 36.91 -23 41 27.4           ~ 49 0
34 GRB 060116 gB 05 38 46.170 -05 26 15.08           ~ 86 0
35 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
36 GRB 140213A gB 07 00 37.18 -73 08 14.1           ~ 102 0
37 GRB 071020 gB 07 58 39.65 +32 51 38.8           ~ 158 0
38 GRB 080516 gB 08 02 34.16 -26 09 35.3           ~ 59 0
39 GRB 141121A gB 08 10 40.68 +22 13 02.7           ~ 108 0
40 Fermi bn120118709 gB 08 19 29.05 -07 11 05.1           ~ 87 0
41 GRB 150323A gB 08 32 42.73 +45 27 52.9           ~ 68 0
42 GRB 051016B gB 08 48 27.810 +13 39 20.00 20.45         ~ 153 0
43 Fermi bn100704149 gB 08 54 33.92 -24 12 09.7           ~ 103 0
44 GRB 130408A gB 08 57 37.30 -32 21 38.9           ~ 98 0
45 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
46 GRB 050505 gB 09 27 03.300 +30 16 23.70     20.74     ~ 206 0
47 Fermi bn090519881 gB 09 29 16.20 +00 11 23.9           ~ 98 0
48 GRB 061021 gB 09 40 36.120 -21 57 05.40 18.21 19.20 16.82     ~ 160 0
49 Fermi bn140206304 gB 09 41 16.90 +66 45 42.7           ~ 149 0
50 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
51 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
52 GRB 171222A gB 09 53 06.69 +35 37 36.1           ~ 57 0
53 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
54 Fermi bn111228657 gB 10 00 16.04 +18 17 52.2           ~ 201 0
55 GRB 150424A gB 10 09 13.35 -26 37 51.2           ~ 94 0
56 GRB 170202A gB 10 10 06 +05 01.0           ~ 90 0
57 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
58 GRB 111123A gB 10 19 23.17 -20 38 41.9           ~ 83 0
59 GRB 180325A gB 10 29 42.57 +24 27 48.7           ~ 85 0
60 Fermi bn120712571 gB 11 18 21.16 -20 02 01.1           ~ 90 0
61 GRB 080603B gB 11 46 07.46 +68 03 38.5           ~ 153 0
62 Fermi bn100615083 gB 11 48 49.25 -19 28 52.2           ~ 133 0
63 GRB 090530 gB 11 57 36.00 +26 35 23.0           ~ 89 0
64 GRB 161108A gB 12 03 09.10 +24 52 05.5           ~ 46 0
65 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
66 Fermi bn170705115 gB 12 49 +17.9           ~ 66 0
67 GRB 160227A gB 12 59 13.71 +78 40 45.1           ~ 69 0
68 GRB 100302A gB 13 02 03.66 +74 35 22.5           ~ 83 0
69 Fermi bn121211574 gB 13 02 07.99 +30 08 54.6           ~ 99 0
70 Fermi bn130420313 gB 13 04 25.49 +59 25 26.8           ~ 112 0
71 GRB 070208 gB 13 11 32.607 +61 57 54.37 20.79 20.79 19.86     ~ 119 0
72 Fermi bn120811649 gB 13 18 43.82 +62 18 02.8           ~ 113 0
73 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
74 GRB 100424A gB 13 57 47.46 +01 32 20.3           ~ 71 0
75 GRB 120521C gB 14 17 09.10 +42 08 39.8           ~ 93 0
76 GRB 090205 gB 14 43 40.00 -27 50 51.4           ~ 99 0
77 GRB 060814 gB 14 45 21.480 +20 35 11.80           ~ 241 0
78 Fermi bn160804065 gB 14 46 31.20 +09 59 56.1           ~ 79 0
79 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 180 0
80 GRB 140518A gB 15 09 00.60 +42 25 05.6           ~ 68 0
81 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
82 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
83 Fermi bn120922939 gB 15 38 59.67 -20 10 55.0           ~ 88 0
84 GRB 120404A gB 15 40 02.29 +12 53 06.3           ~ 104 0
85 GRB 110715A gB 15 50 44.090 -46 14 06.53           ~ 120 0
86 GRB 060502A gB 16 03 42.480 +66 36 02.49     18.65     ~ 143 0
87 GRB 120327A gB 16 27 27.49 -29 24 53.8           ~ 116 0
88 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
89 GRB 140629A gB 16 35 54.44 +41 52 36.7           ~ 89 0
90 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 185 0
91 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 198 0
92 Fermi bn130612141 gB 17 19 10.63 +16 43 11.8           ~ 89 0
93 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
94 GRB 050814 gB 17 36 45.390 +46 20 21.60           ~ 166 0
95 GRB 090418A gB 17 57 15.17 +33 24 21.1           ~ 101 0
96 Fermi bn151027166 gB 18 09 56.87 +61 21 12.3           ~ 143 0
97 Fermi bn120326056 gB 18 15 37.06 +69 15 35.4           ~ 188 0
98 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
99 Fermi bn140512814 gB 19 17 28.81 -15 05 39.5           ~ 133 0
100 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
101 GRB 130514A gB 19 45 07.33 -07 58 41.1           ~ 82 0
102 Fermi bn121128212 gB 20 02 23.88 +54 17 59.1           ~ 128 0
103 Fermi bn080905705 gB 20 06 57.93 -62 33 46.8           ~ 119 0
104 GRB 050315 gB 20 25 54.100 -42 36 02.19           ~ 225 0
105 GRB 150403A gB 20 46 01.17 -62 42 40.1           ~ 116 0
106 GRB 070508 gB 20 51 11.810 -78 23 04.88     19.62     ~ 144 0
107 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 204 0
108 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
109 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
110 GRB 161117A gB 21 28 12.59 -29 36 49.9           ~ 74 0
111 GRB 060605 gB 21 28 37.320 -06 03 31.30   20.12 16.53     ~ 210 0
112 GRB 060522 gB 21 31 44.850 +02 53 10.80           ~ 140 0
113 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
114 GRB 051109A gB 22 01 15.320 +40 49 23.70   20.09 20.14     ~ 190 0
115 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1
116 Fermi bn090927422 gB 22 55 53.41 -70 58 49.3           ~ 112 0
117 GRB 131030A gB 23 00 16.14 -05 22 05.2           ~ 126 0
118 GRB 131103A gB 23 15 40.55 -44 38 25.4           ~ 44 0
119 Fermi bn080810549 gB 23 47 08.00 +00 18 35.1           ~ 240 0
120 GRB 060707 gB 23 48 19.000 -17 54 17.00     19.79     ~ 170 0
121 GRB 061222A gB 23 53 03.419 +46 31 58.60           ~ 177 0

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