2025A&A...694A.194F


Query : 2025A&A...694A.194F

2025A&A...694A.194F - Astronomy and Astrophysics, volume 694A194 (2025/2-1)

Separating deterministic and stochastic gravitational wave signals in realistic pulsar timing array datasets.

FERRANTI I., SHAIFULLAH G., CHALUMEAU A. and SESANA A.

Abstract (from CDS):

Recent observations by pulsar timing arrays (PTAs) suggest the presence of gravitational wave (GW) signals that potentially originate from supermassive black hole binaries (SMBHBs). These binaries can generate two kinds of signals: a stochastic gravitational wave background (GWB) or a deterministic continuous gravitational wave (CGW). The ability to correctly recognize and separate them is crucial for accurate signal recovery and astrophysical interpretation. This paper is aimed at investigating the interaction between stochastic GWB and deterministic CGW signals with the analysis pipelines currently available. We focus on understanding potential misinterpretations and biases in the parameter estimation when these signals are analysed separately or altogether. To this end, we performed several realistic simulations based on the European PTA 24.8 yr dataset. We first injected either a GWB or a CGW into five datasets (of three GWB realisations and two CGW realisations) with identical noise. We analysed each signal type independently and then we analysed data sets containing both a stochastic GWB and a single resolvable CGW. We compared the parameter estimations using different search models, including Earth term (ET) only or combined Earth and pulsar term (ET + PT) CGW templates, along with correlated or uncorrelated power law GWB templates. We show that when searched for independently, the GWB and CGW signals can be misinterpreted (i.e. they can be confused with each other) and only a combined search is able to recover the true signal present. For datasets containing both a GWB and a CGW, failure to account for the latter biases the recovery of the GWB; however, when we perform a combined search, both GWB and CGW parameters can be recovered without any strong bias. Care must be taken with the method used to perform combined searches on these multi-component datasets, as the CGW PT can be misinterpreted as a common uncorrelated red noise. However, this can be avoided by conducting direct searches for a correlated GWB plus a CGW (ET + PT). Our study underscores the importance of combined searches to ensure unbiased recovery of GWB parameters in the presence of strong CGWs. This is crucial to accurately interpreting the signal recently found in PTA data and it is a first step towards a robust framework for disentangling stochastic and deterministic GW components in more sensitive datasets in the future.

Abstract Copyright: © The Authors 2025

Journal keyword(s): black hole physics - gravitational waves - methods: data analysis - pulsars: general

Simbad objects: 27

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Number of rows : 27
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 ACO S 373 ClG 03 38 29.4 -35 27 08           ~ 2029 0
3 PSR B0613-02.0 Psr 06 13 43.977070 -02 00 47.34294           ~ 319 1
4 PSR J0751+1807 Psr 07 51 09.1539 +18 07 38.335           ~ 316 1
5 PSR J0900-3144 Psr 09 00 43.95220 -31 44 30.8722           ~ 68 0
6 PSR J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 419 1
7 PSR J1022+10 Psr 10 22 57.990 +10 01 52.92           ~ 279 2
8 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 286 1
9 NAME Virgo Cluster ClG 12 30 47.8 +12 23 07           ~ 7107 0
10 PSR J1455-3300 Psr 14 55 47.976991 -33 30 46.40280           ~ 165 1
11 PSR J1600-3053 Psr 16 00 51.902514 -30 53 49.45343           ~ 218 0
12 PSR J1640+2224 Psr 16 40 16.744850 +22 24 08.84119           ~ 210 0
13 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
14 PSR J1730-2304 Psr 17 30 21.68471 -23 04 31.2590           ~ 194 1
15 PSR J1738+0333 Psr 17 38 53.966386 +03 33 10.87200           ~ 191 1
16 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
17 PSR J1751-2857 Psr 17 51 32.686848 -28 57 46.57130           ~ 65 1
18 PSR J1801-1417 Psr 18 01 51.064902 -14 17 34.54980           ~ 45 0
19 PSR J1804-27 Psr 18 04 21.13307 -27 17 31.3370           ~ 87 1
20 PSR J1843-1113 Psr 18 43 41.260405 -11 13 31.10310           ~ 86 0
21 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
22 PSR J1909-3744 Psr 19 09 47.42820 -37 44 14.7740           ~ 343 2
23 PSR J1910+1256 Psr 19 10 09.701454 +12 56 25.48680           ~ 108 1
24 PSR J1911+1347 Psr 19 11 55.204694 +13 47 34.38383           ~ 72 0
25 PSR J1918-0642 Psr 19 18 48.027685 -06 42 34.95735           ~ 146 0
26 PSR J2124-3358 Psr 21 24 43.834930 -33 58 45.49195           ~ 337 1
27 PSR J2322+2057 Psr 23 22 22.320041 +20 57 02.50080           ~ 129 1

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