# Resonant Decay of Gravitational Waves into Dark Energy

**Authors:** Paolo Creminelli, Giovanni Tambalo, Filippo Vernizzi, Vicharit, Yingcharoenrat

arXiv: 1906.07015 · 2019-10-31

## TL;DR

This paper investigates how gravitational waves decay into dark energy fluctuations within scalar-tensor theories, revealing potential observable effects on gravitational wave signals detectable by LIGO/Virgo and LISA.

## Contribution

It provides an analytical study of gravitational wave decay into dark energy fluctuations, highlighting the impact of specific operators and the potential for observational detection.

## Key findings

- Resonance effects can significantly modify gravitational wave signals.
- Observable modifications are predicted within specific parameter ranges for current and future detectors.
- Self-interactions of dark energy fluctuations influence the instability and decay process.

## Abstract

We study the decay of gravitational waves into dark energy fluctuations $\pi$, taking into account the large occupation numbers. We describe dark energy using the effective field theory approach, in the context of generalized scalar-tensor theories. When the $m_3^3$ (cubic Horndeski) and $\tilde m_4^2$ (beyond Horndeski) operators are present, the gravitational wave acts as a classical background for $\pi$ and modifies its dynamics. In particular, $\pi$ fluctuations are described by a Mathieu equation and feature instability bands that grow exponentially. Focusing on the regime of small gravitational-wave amplitude, corresponding to narrow resonance, we calculate analytically the produced $\pi$, its energy and the change of the gravitational-wave signal. The resonance is affected by $\pi$ self-interactions in a way that we cannot describe analytically. This effect is very relevant for the operator $m_3^3$ and it limits the instability. In the case of the $\tilde m_4^2$ operator self-interactions can be neglected, at least in some regimes. The modification of the gravitational-wave signal is observable for $3 \times 10^{-20} \lesssim \alpha_{\rm H} \lesssim 10^{-17}$ with a LIGO/Virgo-like interferometer and for $10^{-16} \lesssim \alpha_{\rm H} \lesssim 10^{-10}$ with a LISA-like one.

## Full text

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## Figures

9 figures with captions in the complete paper: https://tomesphere.com/paper/1906.07015/full.md

## References

42 references — full list in the complete paper: https://tomesphere.com/paper/1906.07015/full.md

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Source: https://tomesphere.com/paper/1906.07015