2024MNRAS.527.2214S


Query : 2024MNRAS.527.2214S

2024MNRAS.527.2214S - Mon. Not. R. Astron. Soc., 527, 2214-2231 (2024/January-2)

Solving the inverse cosmological calibration problem of gamma-ray bursts.

SHIROKOV S.I., GAINUTDINOV R.I., LOVYAGIN N.Y. and GOROKHOV V.L.

Abstract (from CDS):

We have received a new physical characteristics fitting based on actual observational data from the Swift mission's long-duration gamma-ray bursts (LGRBs). We considered such characteristics as the Amati parameters for linear correlation (Eiso-Ep,i) and the k-correction for gravitational lensing and Malmquist bias (GLMB) effect. We used the Pantheon SN Ia catalogue and the standard Lambda cold dark matter model with a fixed Hubble constant of H0 = 70 km s–1 Mpc–1 as the baseline for the Hubble function μ(z). In our paper, we formulated the inverse cosmological calibration problem (ICCP) in the non-parametric statistics framework. The ICCP involves fitting non-observable physical characteristics while assuming a fixed cosmological model. To solve this problem, we developed a new method that is resistant to non-Gaussian processes. This method is based on error propagation through the Monte Carlo method and the Theil-Sen method for linear regression estimate. We have demonstrated the stability and robustness of this assessment method. The parameter estimates are as follows: $a=0.92^{+0.12}_{-0.12}$, $b=50.32^{+0.33}_{-0.32}$ without considering the GLMB effect, and $a=0.63^{+0.13}_{-0.14}$, $b=50.12^{+0.33}_{-0.31}$, and $k=1.98^{+0.25}_{-0.24}$ with the effect included. The proposed method can be applied to any other calibration sample of known standard candles, a calibrated sample of LGRBs, and the Hubble function μ(z). In the future, the ICCP idea can be used as an alternative cosmological test for estimating cosmological parameters, including the GLMB effect, or even for the selection of models, providing new information about the Universe. This can be done by analysing the residual values of observational data within the Bayesian statistics paradigm.

Abstract Copyright: © 2023 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): cosmological parameters - distance scale - gamma-ray bursts

Status at CDS : Large table(s) will be appraised for possible ingestion in VizieR.

Simbad objects: 174

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Number of rows : 174
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 101225A gB 00 00 47.48 +44 36 01.0           ~ 163 0
2 GRB 150910A gB 00 22 40.14 +33 28 22.4           ~ 79 0
3 SDSS J002243.71-001657.5 G 00 22 43.71720 -00 16 57.5256           ~ 69 0
4 GRB 170607A gB 00 29 27.84 +09 14 35.5           ~ 62 0
5 GRB 150206A gB 00 40 17.57 -63 10 56.0           ~ 55 0
6 SN 2010ma SN* 00 48 55.35 -34 33 59.5           SNIc 190 1
7 GRB 111225A gB 00 52 37.22 +51 34 19.5           ~ 66 0
8 GRB 121201A gB 00 53 52.21 -42 56 34.5           ~ 49 0
9 GRB 181020A gB 00 55 55.77 -47 22 50.6           ~ 61 0
10 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
11 Fermi bn100814160 gB 01 29 53.61 -17 59 43.6           ~ 219 0
12 Fermi bn091208410 gB 01 57 38.50 +16 52 50.7           ~ 220 0
13 GRB 190106A gB 01 59 31.23 +23 50 43.8           ~ 66 0
14 Fermi bn140304557 gB 02 02 33.90 +33 28 27.9           ~ 106 0
15 Fermi bn090113778 gB 02 08 16.00 +33 26 08.4           ~ 92 0
16 GRB 091018 gB 02 08 46 -57 33.0           ~ 169 0
17 GRB 170714A gB 02 17 17 +01 58.0           ~ 50 0
18 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
19 GRB 151029A gB 02 34 06.71 -35 23 07.8           ~ 40 0
20 GRB 141212A G 02 36 29.9570 +18 08 47.228           ~ 70 0
21 GRB 171020A gB 02 36 59.62 +15 12 14.6           ~ 28 0
22 GRB 140710A gB 02 44 16.26 +35 29 56.7           ~ 46 0
23 Fermi bn130925164 gB 02 44 42.38 -26 09 15.8           ~ 184 0
24 SN 2013ez SN* 02 53 56.70 +13 23 13.6           ~ 118 0
25 Fermi bn100728439 gB 02 56 13.44 +00 16 51.6           ~ 142 0
26 GRB 141026A gB 02 56 20.29 +26 55 42.4           ~ 60 0
27 SN 2019oyw SN* 02 58 10.510 -08 57 27.20           ~ 218 0
28 GRB 191011A gB 02 58 54.70 -27 50 43.4           ~ 38 0
29 GRB 120802A gB 02 59 22.04 +13 46 05.0           ~ 76 0
30 Fermi bn090926914 gB 03 05 14.30 -38 59 50.9           ~ 149 1
31 GRB 140907A gB 03 12 34.98 +46 36 17.2           ~ 81 0
32 GRB 100902A gB 03 14 30 +30 58.2           ~ 68 0
33 GRB 191004B gB 03 16 48.97 -39 38 06.3           ~ 32 0
34 GRB 190324A gB 03 18 27.77 -47 12 54.1           ~ 35 0
35 GRB 181010A gB 03 30 16.88 -23 02 17.9           ~ 39 0
36 GRB 110808A gB 03 49 04.28 -44 11 40.3           ~ 64 0
37 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 168 0
38 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 127 0
39 Fermi bn170113420 gB 04 06 59 -71 56.0           ~ 64 0
40 GRB 121027A gB 04 14 23.450 -58 49 47.17           ~ 136 0
41 GRB 190114A gB 04 22 10.54 +02 11 29.1           ~ 47 0
42 GRB 090407 gB 04 35 54.98 -12 40 45.5           ~ 87 0
43 GRB 140301A gB 04 38 13.81 -34 15 24.3           ~ 48 0
44 Fermi bn120907017 gB 04 58 59.99 -09 18 53.7           ~ 89 0
45 GRB 151027B gB 05 04 52.67 -06 27 00.7           ~ 61 0
46 GRB 111229A gB 05 05 08.86 -84 42 39.1           ~ 47 0
47 Fermi bn141004973 gB 05 06 56.11 +12 49 10.1           ~ 75 0
48 GRB 180329B gB 05 31 36.91 -23 41 27.4           ~ 49 0
49 GRB 151031A gB 05 32 47.02 -39 07 18.7           ~ 27 0
50 Fermi bn150301818 gB 05 56 40.04 -57 58 10.4           ~ 67 0
51 GRB 110801A gB 05 57 44.87 +80 57 21.1           ~ 90 0
52 SN 2016jca SN* 06 06 51.36 -26 47 29.7           SNIc 140 0
53 GRB 151215A gB 06 14 20.20 +35 30 58.3           ~ 47 0
54 Fermi bn180314030 gB 06 37 03.66 -24 29 46.5           ~ 46 0
55 GRB 140430A gB 06 51 44.58 +23 01 25.5           ~ 81 0
56 GRB 140213A gB 07 00 37.18 -73 08 14.1           ~ 102 0
57 SN 2010bh SN* 07 10 30.63 -56 15 19.7           SNIc 336 1
58 GRB 200205B gB 07 11 09.15 -56 29 15.3       18.56 17.15 ~ 22 0
59 GRB 160121A gB 07 16 21.15 -23 35 31.8           ~ 41 0
60 GRB 110422A gB 07 28 11.21 +75 06 24.0           ~ 113 0
61 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 193 0
62 GRB 141121A gB 08 10 40.68 +22 13 02.7           ~ 108 0
63 Fermi bn120118709 gB 08 19 29.05 -07 11 05.1           ~ 87 0
64 Fermi bn150314205 gB 08 26 40.82 +63 50 03.4           ~ 117 0
65 Fermi bn180205184 gB 08 27 16.72 +11 32 32.6           ~ 60 0
66 GRB 150323A gB 08 32 42.73 +45 27 52.9           ~ 68 0
67 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
68 GRB 110503A gB 08 51 06.31 +52 12 27.7           ~ 115 0
69 Fermi bn100704149 gB 08 54 33.92 -24 12 09.7           ~ 103 0
70 GRB 130408A gB 08 57 37.30 -32 21 38.9           ~ 98 0
71 SN 2012bz SN* 09 07 38.38 +14 01 07.5           SNIb/c 193 1
72 GRB 141109A gB 09 38 07.40 -00 36 28.6           ~ 73 0
73 Fermi bn140206304 gB 09 41 16.90 +66 45 42.7           ~ 149 0
74 GRB 171222A gB 09 53 06.69 +35 37 36.1           ~ 57 0
75 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
76 GRB 130418A gB 09 56 08.86 +13 40 01.8           ~ 70 0
77 Fermi bn111228657 gB 10 00 16.04 +18 17 52.2           ~ 201 0
78 GRB 170202A gB 10 10 06 +05 01.0           ~ 90 0
79 GRB 100219A gB 10 16 48.48 -12 34 00.0           ~ 130 0
80 GRB 191221B gB 10 19 19.17 -38 09 27.5           ~ 66 0
81 GRB 180325A gB 10 29 42.57 +24 27 48.7           ~ 85 0
82 GRB 160203A gB 10 47 48.32 -24 47 20.4           ~ 54 0
83 GRB 170519A gB 10 53 42.49 +25 22 26.7           ~ 55 0
84 GRB 100316B gB 10 54 00 -45 28.0           ~ 62 0
85 GRB 110205A gB 10 58 31.12 +67 31 31.2           ~ 213 0
86 SN 2017iuk SN* 11 09 39.49 -12 35 18.7           SNII 210 0
87 Fermi bn120712571 gB 11 18 21.16 -20 02 01.1           ~ 90 0
88 GRB 100513A gB 11 18 26.83 +03 37 40.8           ~ 74 0
89 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
90 Fermi bn100615083 gB 11 48 49.25 -19 28 52.2           ~ 133 0
91 GRB 090530 gB 11 57 36.00 +26 35 23.0           ~ 89 0
92 GRB 161108A gB 12 03 09.10 +24 52 05.5           ~ 46 0
93 GRB 140318A gB 12 16 21.43 +20 12 32.5           ~ 41 0
94 GRB 140515A gB 12 24 15.48 +15 06 17.7           ~ 90 0
95 GALEX J123205.0-105600 Bz? 12 32 04.9717245480 -10 56 00.722548932         16.421 ~ 186 0
96 GRB 140114A gB 12 34 05.10 +27 57 02.6           ~ 61 0
97 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
98 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
99 GRB 121229A gB 12 40 23.41 -50 35 37.2           ~ 57 0
100 GRB 150413A gB 12 41 35.10 +71 50 21.9           ~ 70 0
101 GRB 140428A gB 12 57 28.45 +28 23 05.7           ~ 35 0
102 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 198 0
103 GRB 160227A gB 12 59 13.71 +78 40 45.1           ~ 69 0
104 Fermi bn141220252 gB 13 00 15.70 +32 08 47.2           ~ 81 0
105 GRB 100302A gB 13 02 03.66 +74 35 22.5           ~ 83 0
106 Fermi bn121211574 gB 13 02 07.99 +30 08 54.6           ~ 99 0
107 Fermi bn130420313 gB 13 04 25.49 +59 25 26.8           ~ 112 0
108 Fermi bn140423356 gB 13 09 06.20 +49 50 18.3           ~ 114 0
109 Fermi bn141221338 gB 13 13 09.02 +08 12 18.3           ~ 76 0
110 Fermi bn120811649 gB 13 18 43.82 +62 18 02.8           ~ 113 0
111 GRB 150727A gB 13 35 52.52 -18 19 32.7           ~ 59 0
112 GRB 140311A gB 13 57 13.29 +00 38 31.7           ~ 86 0
113 GRB 100424A gB 13 57 47.46 +01 32 20.3           ~ 71 0
114 GRB 090529 gB 14 09 52.49 +24 27 33.5           ~ 89 0
115 GRB 120521C gB 14 17 09.10 +42 08 39.8           ~ 93 0
116 GRB 120805A gB 14 26 09.13 +05 49 30.4           ~ 39 0
117 GRB 090205 gB 14 43 40.00 -27 50 51.4           ~ 99 0
118 GRB 150423A gB 14 46 18.96 +12 17 00.6           ~ 79 0
119 Fermi bn160804065 gB 14 46 31.20 +09 59 56.1           ~ 79 0
120 Fermi bn130610133 gB 14 57 40.91 +28 12 25.8           ~ 89 0
121 GRB 140518A gB 15 09 00.60 +42 25 05.6           ~ 68 0
122 GRB 120722A gB 15 21 58.0 +13 15 01           ~ 49 0
123 GRB 140614A gB 15 24 40.69 -79 07 43.8           ~ 43 0
124 Fermi bn120922939 gB 15 38 59.67 -20 10 55.0           ~ 88 0
125 GRB 120404A gB 15 40 02.29 +12 53 06.3           ~ 104 0
126 GRB 110715A gB 15 50 44.090 -46 14 06.53           ~ 120 0
127 GRB 140903A G 15 52 03.2650 +27 36 10.710           ~ 138 0
128 GRB 090814A gB 15 58 26.44 +25 37 52.4           ~ 56 0
129 GRB 190719C gB 16 00 49.50 +13 00 00.6           ~ 43 0
130 GRB 190627A gB 16 19 18.73 -05 17 20.4           ~ 43 0
131 GRB 120724A gB 16 20 46.0 +03 30 33           ~ 51 0
132 GRB 120327A gB 16 27 27.49 -29 24 53.8           ~ 116 0
133 GRB 181213A gB 16 33 04.83 +78 29 49.1           ~ 24 0
134 GRB 090726 gB 16 34 43.50 +72 51 56.5           ~ 70 0
135 GRB 140629A gB 16 35 54.44 +41 52 36.7           ~ 89 0
136 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 185 0
137 GRB 200829A gB 16 44 49.42 +72 19 45.3           ~ 55 0
138 SN 2018fip SN* 16 54 15.64 -54 02 39.5           SNIc-BL 83 0
139 Fermi bn170903534 gB 16 58 06.22 +34 58 44.6           ~ 42 0
140 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 198 0
141 Fermi bn130612141 gB 17 19 10.63 +16 43 11.8           ~ 89 0
142 Fermi bn120326056 gB 18 15 37.06 +69 15 35.4           ~ 188 0
143 GRB 120815A gB 18 15 54.40 -52 07 29.0           ~ 103 0
144 GRB 120909A gB 18 22 56.81 -59 26 54.9           ~ 103 0
145 Fermi bn140506880 gB 18 27 06.04 -55 38 08.7           ~ 113 0
146 GRB 160425A gB 18 41 18.56 -54 21 36.1           ~ 49 0
147 GRB 110726A gB 19 06 52.21 +56 04 16.4           ~ 55 0
148 GRB 170531B gB 19 07 31.99 -16 25 09.3           ~ 38 0
149 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
150 Fermi bn131004904 gB 19 44 27.20 -02 57 31.0           ~ 113 0
151 GRB 130514A gB 19 45 07.33 -07 58 41.1           ~ 82 0
152 GRB 100425A gB 19 56 47.16 -26 25 50.5           ~ 91 0
153 Fermi bn121128212 gB 20 02 23.88 +54 17 59.1           ~ 128 0
154 GRB 181110A gB 20 09 16.32 -36 53 48.2           ~ 45 0
155 GRB 150403A gB 20 46 01.17 -62 42 40.1           ~ 116 0
156 GRB 130427B gB 20 59 36.00 -22 32 51.6           ~ 60 0
157 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 204 0
158 Fermi bn161129300 gB 21 04 54.66 +32 08 05.5           ~ 65 0
159 GRB 140622A gB 21 08 41.56 -14 25 09.5           ~ 61 0
160 Fermi bn110818860 gB 21 09 20.890 -63 58 51.80           ~ 92 0
161 GRB 161117A gB 21 28 12.59 -29 36 49.9           ~ 74 0
162 GRB 090809 gB 21 54 43.2 -00 05 02           ~ 90 0
163 GRB 131117A gB 22 09 19.47 -31 45 44.5           ~ 67 0
164 GRB 161014A gB 22 10 35.42 +07 28 07.6           ~ 69 0
165 Fermi bn150821406 gB 22 47 39.15 -57 53 38.2           ~ 71 0
166 GRB 170604A gB 22 50 37.49 -15 24 44.6           ~ 37 0
167 Fermi bn090927422 gB 22 55 53.41 -70 58 49.3           ~ 112 0
168 GRB 131030A gB 23 00 16.14 -05 22 05.2           ~ 126 0
169 GRB 131103A gB 23 15 40.55 -44 38 25.4           ~ 44 0
170 Fermi bn100816026 gB 23 26 57.56 +26 34 42.6           ~ 170 0
171 SN 2012eb SN* 23 41 38.35 -46 11 07.0           SNIb/c 62 1
172 GRB 130701A gB 23 48 55.05 +36 06 01.2           ~ 81 0
173 Fermi bn180620660 gB 23 50 05.07 -57 57 44.7           ~ 53 0
174 SN 2013fu SN* 23 54 29.91 +29 25 47.6           SNIb/c 144 1

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