2025ApJ...990...85D


Query : 2025ApJ...990...85D

2025ApJ...990...85D - Astrophys. J., 990, 85 (2025/September-1)

Choosing Suitable Noise Models for Nanohertz Gravitational-wave Astrophysics.

DI MARCO V., ZIC A., SHANNON R.M., THRANE E. and KULKARNI A.D.

Abstract (from CDS):

Accurately estimating the parameters of the nanohertz gravitational-wave background is essential for understanding its origin. The background is typically modeled with a power-law spectrum, parameterized with an amplitude A, which describes its intensity, and a spectral index γ, which describes how the background varies with frequency. Different collaborations have produced varied estimates of γ, some in tension with the value of γ = 13/3 expected for circular, gravitational-wave-driven binary black holes. However, estimates of A and γ can be affected by systematic errors and misspecified noise models. We investigate how systematic errors-which may plausibly be present in pulsar timing analyses-can shift inferences about A, γ. We demonstrate that conservatively incorporating noise sources into the model that are not actually present in the data does not produce bias inferences in practice. This addresses concerns that an overly complex noise model might lead to bias from a needlessly conservative prior. Our results highlight the importance of using comprehensive noise models in pulsar timing analyses to ensure accurate and reliable parameter estimation of the gravitational-wave background.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Gravitational waves - Astronomy data analysis

Simbad objects: 30

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Number of rows : 30
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 PSR J0030+0451 Psr 00 30 27.42348 +04 51 39.7144           ~ 596 1
2 PSR J0125-23 Psr 01 25 01.075151 -23 27 08.13167           ~ 20 0
3 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
4 PSR B0613-02.0 Psr 06 13 43.977070 -02 00 47.34294           ~ 319 1
5 PSR J0614-3329 Psr 06 14 10.3479 -33 29 54.116           ~ 134 1
6 PSR J0712-68 Psr 07 11 54.153093 -68 30 47.23387           ~ 120 1
7 PSR J0900-3144 Psr 09 00 43.95220 -31 44 30.8722           ~ 68 0
8 PSR J1017-7156 Psr 10 17 51.311783 -71 56 41.57398           ~ 61 1
9 PSR J1022+10 Psr 10 22 57.990 +10 01 52.92           ~ 279 2
10 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 286 1
11 PSR J1045-45 Psr 10 45 50.179671 -45 09 54.05686           ~ 154 1
12 PSR J1125-6014 Psr 11 25 55.243299 -60 14 06.80942           ~ 61 0
13 PSR J1446-4701 Psr 14 46 35.709721 -47 01 26.79678           ~ 82 1
14 PSR J1545-4550 Psr 15 45 55.945403 -45 50 37.50813           ~ 34 0
15 PSR J1600-3053 Psr 16 00 51.902514 -30 53 49.45343           ~ 218 0
16 PSR J1604-72 Psr 16 03 35.670781 -72 02 32.82328           ~ 142 0
17 PSR J1643-1224 Psr 16 43 38.16612 -12 24 58.6334           ~ 260 2
18 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
19 PSR J1730-2304 Psr 17 30 21.68471 -23 04 31.2590           ~ 194 1
20 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
21 PSR J1832-0836 Psr 18 32 27.589497 -08 36 55.14540           ~ 86 0
22 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
23 PSR J1902-5105 Psr 19 02 02.8476 -51 05 56.969           ~ 64 0
24 PSR J1909-3744 Psr 19 09 47.42820 -37 44 14.7740           ~ 343 2
25 PSR J1933-6210 Psr 19 33 32.413330 -62 11 46.69324           ~ 48 0
26 PSR B1937+21.4 Psr 19 39 38.560096 +21 34 59.13552           ~ 1142 0
27 PSR J2124-3358 Psr 21 24 43.834930 -33 58 45.49195           ~ 337 1
28 PSR J2129-5718 Psr 21 29 22.781548 -57 21 14.33356           ~ 122 1
29 PSR B2145-07.8 Psr 21 45 50.45590 -07 50 18.5900           ~ 336 0
30 PSR J2241-5236 Psr 22 41 42.03161 -52 36 36.2492           ~ 143 1

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