2025A&A...698A.215G

Query : 2025A&A...698A.215G

2025A&A...698A.215G - Astronomy and Astrophysics, volume 698A215 (2025/6-1)

Measuring the Hubble constant using localized and nonlocalized fast radio bursts.

GAO D.H., WU Q., HU J.P., YI S.X., ZHOU X., WANG F.Y. and DAI Z.G.

Abstract (from CDS):

The Hubble constant (H0) is one of the most important parameters in the standard ΛCDM model. The measurements given by the main two methods show a gap larger than 4σ, which is known as Hubble tension. Fast radio bursts (FRBs) are extragalactic pulses with durations of milliseconds. They can be used as cosmological probes. We constrain H0 using localized and nonlocalized FRBs. We first used 108 localized FRBs to constrain H0 using the probability distributions of DMhost and DMIGM from the IllustrisTNG simulation. Then, we used a Monte Carlo sampling to calculate the pseudo-redshift distributions of 527 nonlocalized FRBs from CHIME observations. The 108 localized FRBs yield a constraint of $ H_0 = 69.40_{-1.97}^{+2.14} $ km s–1 Mpc–1, which lies between the early- and late-time values. The constraint of H0 from nonlocalized FRBs yields $ H_0 = 68.81_{-0.68}^{+0.68} $ km s–1 Mpc–1. This result indicates that the uncertainty on the constraint of H0 drops to ∼1% when the number of localized FRBs is increased to ∼500. These uncertainties only include the statistical error. The systematic errors are also discussed and play a dominant role in the current sample.

Abstract Copyright: © The Authors 2025

Journal keyword(s): cosmological parameters

Simbad objects: 97

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Number of rows : 97
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 FRB 20200223B rB 00 28 16.800 +29 00 36.00           ~ 25 0
2 FRB 20240210A rB 00 39 55.040 -27 39 34.78           ~ 12 0
3 FRB 20210603A rB 00 41 05.774 +21 13 34.57           ~ 17 0
4 FRB 20240310A rB 01 10 57.700 -44 24 05.24           ~ 10 0
5 FRB 20220918A rB 01 10 57.900 -70 47 05.90           ~ 10 0
6 FRB 20220529A rB 01 16 25.014 +20 37 56.60           ~ 15 0
7 FRB 20221116A rB 01 24 50.450 +72 39 14.10           ~ 14 0
8 FRB 20230526A rB 01 29 27.500 -52 46 07.70           ~ 12 0
9 FRB 20180916B rB 01 58 00.750 +65 43 00.30           ~ 457 0
10 FRB 20220319D rB 02 08 42.700 +71 02 06.94           ~ 39 0
11 FRB 20230902A rB 03 29 28.100 -47 33 45.50           ~ 9 0
12 FRB 200906 rB 03 33 59.08 -14 04 59.5           ~ 43 0
13 FRB 20221106A rB 03 46 38.100 -25 39 44.90           ~ 12 0
14 FRB 20190614D rB 04 20 18.13 +73 42 24.3           ~ 37 0
15 NAME FRB 180814.J0422+73 rB 04 22 44.0 +73 39 52           ~ 112 0
16 FRB 20190418A rB 04 23 09.6000 +16 02 24.000           ~ 25 0
17 FRB 20240123A rB 04 24 32.161 +71 35 47.37           ~ 10 0
18 FRB 20221113A rB 04 45 38.640 +70 18 26.60           ~ 14 0
19 FRB 20220726A rB 04 55 46.960 +69 55 44.80           ~ 16 0
20 FRB 20201124A rB 05 07 57.600 +26 11 24.00           ~ 307 0
21 FRB 20181119D rB 05 31 58.6980 +33 08 52.588           ~ 933 0
22 FRB 180301 rB 06 12 43.40 +04 33 44.8           ~ 125 0
23 FRB 20231220A rB 08 08 49.305 +71 43 18.17           ~ 10 0
24 FRB 20230718A rB 08 32 38.804 -40 27 06.33           ~ 12 0
25 FRB 20221027A rB 08 43 29.230 +72 06 03.50           ~ 14 0
26 FRB 20220310F rB 08 58 52.920 +73 29 27.00           ~ 25 0
27 FRB 20221029A rB 09 27 51.220 +72 27 08.34           ~ 15 0
28 FRB 20231120A rB 09 35 56.150 +73 17 04.80           ~ 16 0
29 FRB 20200120E rB 09 57 56.7 +68 49 32           ~ 219 0
30 FRB 20240201A rB 10 01 49.110 +13 54 48.53           ~ 12 0
31 FRB 20231226A rB 10 21 07.600 +06 07 45.90           ~ 11 0
32 FRB 20230216A rB 10 25 53.320 +03 26 12.57           ~ 12 0
33 FRB 211212 rB 10 30 40.700 +01 40 36.80           ~ 30 0
34 NAME FRB 181030.J1054+73 rB 10 33 24.0000 +73 47 24.000           ~ 79 0
35 FRB 20240213A rB 10 35 02.703 +71 46 31.29           ~ 10 0
36 FRB 20220330D rB 10 55 00.300 +70 21 02.70           ~ 15 0
37 FRB 20230628A rB 11 07 08.810 +72 16 54.64           ~ 16 0
38 FRB 20230712A rB 11 09 26.050 +72 33 28.02           ~ 13 0
39 FRB 20240229A rB 11 34 56.311 +71 47 01.68           ~ 10 0
40 FRB 20230307A rB 11 51 07.520 +71 41 44.30           ~ 14 0
41 FRB 20181223C rB 12 04 12.0000 +27 34 48.000           ~ 24 0
42 FRB 190714 rB 12 15 55.1 -13 01 16           ~ 64 0
43 FRB 20191106C rB 13 18 +43.0           ~ 22 0
44 FRB 211127 rB 13 19 09.500 -18 49 28.40           ~ 32 0
45 FRB 210320 rB 13 37 16.800 -15 24 37.30           ~ 29 0
46 FRB 211203 rB 13 37 52.800 -31 22 04.00           ~ 20 0
47 FRB 190523 rB 13 48 15.6 +72 28 11           ~ 109 0
48 FRB 20190303A G 13 51 59.77 +48 06 57.6           ~ 58 0
49 FRB 20220105A rB 13 55 12.94 +22 27 59.4           ~ 19 0
50 FRB 20240119A rB 14 32 28.067 +71 45 19.55           ~ 10 0
51 FRB 20220418A rB 14 36 25.340 +70 05 45.40           ~ 24 0
52 FRB 200430 rB 15 18 49.54 +12 22 36.8           ~ 59 0
53 FRB 20230124A rB 15 27 39.900 +70 58 05.20           ~ 15 0
54 FRB 20230626A rB 15 42 31.100 +71 08 00.77           ~ 14 0
55 FRB 20220920A rB 16 01 01.700 +70 55 07.68           ~ 28 0
56 FRB 20190520B rB 16 02 04.270 -11 17 17.32           ~ 211 0
57 FRB 20231123B rB 16 10 09.160 +70 47 06.20           ~ 14 0
58 FRB 20190110C rB 16 27 55.2000 +41 25 12.000           ~ 36 0
59 FRB 20210405I rB 17 01 21.50 -49 32 42.8           ~ 17 0
60 FRB 20190425A rB 17 02 41.0 +21 34 34           ~ 47 0
61 FRB 20221219A rB 17 10 31.150 +71 37 36.63           ~ 19 0
62 FRB 20201123A rB 17 34 40.560 -50 46 02.00           ~ 12 0
63 FRB 20240215A rB 17 53 43.990 +71 39 14.28           ~ 10 0
64 FRB 20220204A rB 18 16 54.300 +69 43 21.01           ~ 15 0
65 FRB 20221012A rB 18 43 11.690 +70 31 27.15           ~ 25 0
66 FRB 20220914A rB 18 48 13.630 +73 20 12.89           ~ 31 0
67 FRB 20220509G rB 18 50 40.800 +70 14 37.80           ~ 37 0
68 FRB 20220717A rB 19 33 13.00 -19 17 15.8           ~ 8 0
69 FRB 210807 rB 19 56 49.000 -00 48 51.40           ~ 27 0
70 FRB 20230708A rB 20 12 56.900 -55 22 50.40           ~ 14 0
71 FRB 20220207C rB 20 40 47.890 +72 52 56.38           ~ 29 0
72 FRB 20220825A rB 20 47 55.550 +72 35 05.89           ~ 25 0
73 FRB 20220506D rB 21 12 10.760 +72 49 38.20           ~ 24 0
74 FRB 190611 rB 21 22 58.91 -79 23 51.3           ~ 82 0
75 FRB 20240114A rB 21 27 39.8350 +04 19 45.634           ~ 66 0
76 FRB 190102 rB 21 29 39.76 -79 28 32.5           ~ 83 0
77 FRB 20220208A rB 21 30 18.030 +70 02 27.75           ~ 15 0
78 FRB 191001 rB 21 33 24.373 -54 44 51.40           ~ 64 0
79 FRB 20210410D rB 21 44 20.70 -79 19 05.5           ~ 23 0
80 FRB 180924 rB 21 44 25.255 -40 54 00.10           ~ 140 0
81 FRB 181112 rB 21 49 23.630 -52 58 15.39           ~ 131 0
82 FRB 20190711A rB 21 57 40.7 -80 21 29           ~ 114 0
83 FRB 171020 rB 22 15.0 -19 40           ~ 54 0
84 FRB 190608 rB 22 16 04.74 -07 53 53.6           ~ 102 0
85 FRB 20230814A rB 22 23 53.90 +73 01 33.3           ~ 8 0
86 FRB 20220725A rB 22 27 00.000 +34 53 00.00           ~ 13 0
87 FRB 20220831A rB 22 34.8 +70 32           ~ 12 0
88 FRB 20210117A rB 22 39 55.015 -16 09 05.45           ~ 49 0
89 FRB 20230501A rB 22 40 06.520 +70 55 19.82           ~ 14 0
90 FRB 20221101B rB 22 48 51.890 +70 40 52.20           ~ 18 0
91 FRB 191228 rB 22 57 43.30 -29 35 38.7           ~ 37 0
92 FRB 20181220A rB 23 04 26.4000 +48 25 48.000           ~ 26 0
93 FRB 20220912A rB 23 09 04.9 +48 42 25           ~ 126 0
94 FRB 20230521B rB 23 18 42.840 +71 31 19.07           ~ 10 0
95 FRB 20220307B rB 23 23 29.880 +72 11 32.59           ~ 26 0
96 FRB 20220610A rB 23 24 17.569 -33 30 49.37           ~ 31 0
97 FRB 20220501C rB 23 29 50.000 -32 27 00.00           ~ 12 0

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