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Testing Gravity with Realistic Gravitational Waveforms in Pulsar Timing Arrays

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arxiv 2408.11774 v2 pith:IQRNY7IO submitted 2024-08-21 astro-ph.CO gr-qc

Testing Gravity with Realistic Gravitational Waveforms in Pulsar Timing Arrays

classification astro-ph.CO gr-qc
keywords assumptionconsidergravitationalwavesapproximationarraysbackgroundfrequency
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We consider the effects of relaxing the assumption that gravitational waves composing the stochastic gravitational wave background (SGWB) are uncorrelated between frequencies in analyses of the data from Pulsar Timing Arrays (PTAs). While individual monochromatic plane waves are often a good approximation, a background composed of unresolved astrophysical sources cannot be exactly uncorrelated since an infinite plane wave propagates no temporal signal. We consider how relaxing this assumption allows us to extract potential information about modified dispersion relations and other fundamental physics questions, as both the group and phase velocity of waves become relevant. After developing the formalism we carry out simple Gaussian wavepacket examples and then consider more realistic waveforms, such as that from binary inspirals. When the frequency evolves only slowly across the PTA temporal baseline, the monochromatic assumption at an effective mean frequency remains a good approximation and we provide scaling relations that characterize its accuracy.

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Cited by 2 Pith papers

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  1. Notes on gravitational wave amplitude evolution beyond null geodesics

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    A wavevector-divergence formula is derived for GW amplitude transport beyond null geodesics, giving no distortion for constant subluminal group velocity and a frequency-domain-invariant amplitude shift for massive gravitons.

  2. Beyond general relativity: gravitational waves in non-minimally coupled theories

    gr-qc 2025-10 conditional novelty 5.0

    A generalized propagation parameterization for gravitational-wave strains is extended to O(H²) and O(H′), then mapped to Kalb-Ramond, axion-dilaton–Chern-Simons–Gauss-Bonnet, and U(1) dark-photon models.