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    Analysis of the propagation of gravitational radiation under a graviton of nonzero mass: Cosmological constraints without electromagnetic counterparts

    Margaret Johnston*, Marios Kalomenopoulos†, and Carl-Johan Haster‡

    • *Contact author: margaret.johnston@unlv.edu
    • †Contact author: marios.kalomenopoulos@unlv.edu
    • ‡Contact author: carl.haster@unlv.edu

    Phys. Rev. D 112, 083554 – Published 28 October, 2025

    DOI: https://doi.org/10.1103/263g-4vn7

    Abstract

    Under the assumptions of general relativity (GR), gravitational waves (GWs) propagate at the speed of light and their mediation can be represented as a particle through a massless graviton. We investigate the impact and observability of the presence of a massive graviton, how such a modification to GR would also modify the propagation of observed GWs from astrophysical sources, and how this effect can be used as an independent measurement of cosmological parameters. We demonstrate that a massive graviton allows the extraction of redshift information from the GWs signal, and propose a method to constrain cosmology, focusing on the Hubble parameter H0 and matter energy Ωm, with only GWs observations. We simulate the impact of a massive graviton on compact binary coalescence observations in a near-future Laser Interferometer Gravitational Wave Observatory-Virgo-Kamioka Gravitational Wave Detector interferometer network through a modification to the gravitational wave phase in the post-Newtonian framework. Our analysis finds that if we assume the presence of a graviton with a Compton wavelength of λG≈5×1016  m, corresponding to a mass mG≤2.3×10−23  eV/c2, we can utilize a simulated population of 60 binary black hole observations to constrain H0 to a similar precision as current gravitational wave constraints without electromagnetic counterparts (at 90% credible intervals): H0=58−19+34  km s−1  Mpc−1 and Ωm=0.29−0.08+0.10. More sensitive observatories will be necessary to probe lower values in the graviton mass range and fully exploit this method.

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