Testing No slip model with pulsar timing arrays: NANOGrav and IPTA

Abstract We perform an observational study of modified gravity considering a potential inflationary interpretation of pulsar timing arrays (PTA). We use a motivated model known as no slip in which the gravitational wave propagation is modified. Specifically, by using two different parametrizations for the model, we find the approximate transfer functions for tensor perturbations. In this way, we obtain the spectral energy density of gravitational waves and use NANOGrav and IPTA second data release to constrain parameters of the model. In parametrization I, ξ is degenerate with log 10 A and γ and in parametrization II, c M is also degenerate with both log 10 A and γ . For c M , we only get an upper bound on the parameter. Thus, it is difficult to constrain them with percent level accuracy with the current PTA data.

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Publication Details

Journal
Journal of Cosmology and Astroparticle Physics
Published
2024-12-01
DOI
https://doi.org/10.1088/1475-7516/2024/12/045
Primary Topic
Pulsars and Gravitational Waves Research
Type
article
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article

Testing No slip model with pulsar timing arrays: NANOGrav and IPTA

Alireza Allahyari, Shahram Khosravi, Mohammad Mehdi Davari
Journal of Cosmology and Astroparticle Physics
Pulsars and Gravitational Waves Research
article

Testing No slip model with pulsar timing arrays: NANOGrav and IPTA

Alireza Allahyari, Shahram Khosravi, Mohammad Mehdi Davari
article en

Abstract

Abstract We perform an observational study of modified gravity considering a potential inflationary interpretation of pulsar timing arrays (PTA). We use a motivated model known as no slip in which the gravitational wave propagation is modified. Specifically, by using two different parametrizations for the model, we find the approximate transfer functions for tensor perturbations. In this way, we obtain the spectral energy density of gravitational waves and use NANOGrav and IPTA second data release to constrain parameters of the model. In parametrization I, ξ is degenerate with log 10 A and γ and in parametrization II, c M is also degenerate with both log 10 A and γ . For c M , we only get an upper bound on the parameter. Thus, it is difficult to constrain them with percent level accuracy with the current PTA data.

Journal of Cosmology and Astroparticle PhysicsVol. 2024(12)
Kharazmi University (IR)
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Openalex Percentile: Top 83%
Pulsars and Gravitational Waves Research
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Testing No slip model with pulsar timing arrays: NANOGrav and IPTA — Alireza Allahyari, Shahram Khosravi, et al. · Journal of Cosmology and Astroparticle Physics (2024) | TGRS Research Map | TGRS