Source anisotropies and pulsar timing arrays

Pulsar timing arrays (PTAs) hunt for gravitational waves (GWs) by searching for the correlations that GWs induce in the time-of-arrival residuals from different pulsars. If the GW sources are of astrophysical origin, then they are located at discrete points on the sky. However, PTA data are often modeled, and subsequently analyzed, via a “standard Gaussian ensemble.” That ensemble is obtained in the limit of an infinite density of vanishingly weak, Poisson-distributed sources. In this paper, we move away from that ensemble, to study the effects of two types of “source anisotropy.” The first (a), which is often called “shot noise,” arises because there are <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>N</a:mi></a:math> discrete GW sources at specific sky locations. The second (b) arises because the GW source positions are not a Poisson process, for example, because galaxy locations are clustered. Here, we quantify the impact of (a) and (b) on the mean and variance of the pulsar-averaged Hellings and Downs correlation. For conventional PTA sources, we show that the effects of shot noise (a) are much larger than the effects of clustering (b). Published by the American Physical Society 2024

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Publication Details

Journal
Physical review. D/Physical review. D.
Published
2024-12-03
DOI
https://doi.org/10.1103/physrevd.110.123507
Citations
12
Primary Topic
Pulsars and Gravitational Waves Research
Type
article
Field-Weighted Citation Impact
3.98

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article

Source anisotropies and pulsar timing arrays

B. Allen, Serena Valtolina, D. Agarwal, Joseph D. Romano
12 citations
Physical review. D/Physical review. D.
Pulsars and Gravitational Waves Research
3.98
article

Source anisotropies and pulsar timing arrays

B. Allen, Serena Valtolina, D. Agarwal, Joseph D. Romano
article en
12 citations

Abstract

Pulsar timing arrays (PTAs) hunt for gravitational waves (GWs) by searching for the correlations that GWs induce in the time-of-arrival residuals from different pulsars. If the GW sources are of astrophysical origin, then they are located at discrete points on the sky. However, PTA data are often modeled, and subsequently analyzed, via a “standard Gaussian ensemble.” That ensemble is obtained in the limit of an infinite density of vanishingly weak, Poisson-distributed sources. In this paper, we move away from that ensemble, to study the effects of two types of “source anisotropy.” The first (a), which is often called “shot noise,” arises because there are <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>N</a:mi></a:math> discrete GW sources at specific sky locations. The second (b) arises because the GW source positions are not a Poisson process, for example, because galaxy locations are clustered. Here, we quantify the impact of (a) and (b) on the mean and variance of the pulsar-averaged Hellings and Downs correlation. For conventional PTA sources, we show that the effects of shot noise (a) are much larger than the effects of clustering (b). Published by the American Physical Society 2024

Physical review. D/Physical review. D.Vol. 110(12)
Leibniz University Hannover (DE), The University of Texas Rio Grande Valley (US), Max Planck Institute for Gravitational Physics (DE), UCLouvain (BE)
National Science Foundation, University of Texas Rio Grande Valley, Fédération Wallonie-Bruxelles, Fonds Spéciaux de Recherche
Openalex Percentile: Top 6%
Pulsars and Gravitational Waves Research
3.98
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Source anisotropies and pulsar timing arrays — B. Allen, Serena Valtolina, et al. · Physical review. D/Physical review. D. (2024) | TGRS Research Map | TGRS