Abstract
To date, the only limit on graviton mass using galaxy clusters was obtained by Goldhaber and Nieto in 1974, using the fact that the orbits of galaxy clusters are bound and closed, and extend up to 580 kpc. From positing that only a Newtonian potential gives rise to such stable bound orbits, a limit on the graviton mass mg<1.1×10−29eV was obtained [1]. Recently, it has been shown that one can obtain closed bound orbits for Yukawa potential [2], thus invalidating the main ansatz used in Ref. [1] to obtain the graviton mass bound. In order to obtain a revised estimate using galaxy clusters, we use dynamical mass models of the Abell 1689 (A1689) galaxy cluster to check their compatibility with a Yukawa gravitational potential. We use the mass models for the gas, dark matter, and galaxies for A1689 from Refs. [3,4], who used this cluster to test various alternate gravity theories, which dispense with the need for dark matter. We quantify the deviations in the acceleration profile using these mass models assuming a Yukawa potential and that obtained assuming a Newtonian potential by calculating the χ2 residuals between the two profiles. Our estimated bound on the graviton mass (mg) is thereby given by, mg<1.37×10−29eV or in terms of the graviton Compton wavelength of, λg>9.1×1019km at 90% confidence level.
Highlights
A century after its inception, General relativity (GR) passes all observational tests at solar system and binary pulsar length scales with flying colors [5,6,7]
In order to test for the validity of this modified acceleration law, we assume that the total mass is the same as that in Newtonian gravity and we only look for deviations compared to ordinary gravity as a function of distance from the cluster center
In 1974, a limit on graviton mass of mg < 1.1 × 10−29 eV was obtained from galaxy clusters, using the fact that the orbits of galaxy clusters are bound up to 580 kpc [1] and such closed bound orbits can only exist within Newtonian gravity
Summary
A century after its inception, General relativity (GR) passes all observational tests at solar system and binary pulsar length scales with flying colors [5,6,7]. The current best limit (from all the three types of methods) on the mass of a graviton comes from the measurements of weak lensing cosmic shear [59], obtained by comparing the variance of the modified shear convergence power spectrum in massive gravity models to the observed data [60].1. To the best of our knowledge, we are not aware of any direct constraint on graviton mass using galaxy clusters from completed stage II or ongoing stage III dark energy experiments, or any forecast on the estimated sensitivity to graviton mass from upcoming stage IV experiments such as LSST [98], Euclid [99], WFIRST [100], etc This is despite the fact that one of the key science driver for these upcoming surveys is to test modified gravity theories [101].
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