Scalar-induced gravitational waves in spatially covariant gravity with two tensorial degrees of freedom
Author(s)
Feng, Jia-Xi, Yu, Yang, Yu, Yan-Heng, Gao, Xian, Huang, Qing-Guo
Abstract
We study scalar-induced gravitational waves (SIGWs) in a spatially covariant gravity model with two tensorial degrees of freedom, minimally coupled to a $k$-essence scalar field. For the parameter choice considered during radiation domination, the quadratic tensor action coincides with that of general relativity (GR). We derive the scalar transfer functions at finite $σ\equiv C_2\bar N$ and in the large-$|σ|$ limit. We then construct the source function of SIGWs. We further examine a cubic extrinsic-curvature interaction that modifies the source function of SIGWs without affecting the background or quadratic actions. We calculate the fractional energy density of SIGWs for monochromatic and log-normal primordial curvature power spectra. We find that, for the positive values of $σ$ studied, finite-$σ$ effects suppress the spectrum over a broad range of scales relative to the result in the $σ\rightarrow \infty$ limit. In this limit, the cubic interaction suppresses the spectrum at small wavenumbers and enhances it at larger wavenumbers. These results show that modified scalar dynamics and non-linear interactions can alter the fractional energy density of SIGWs even when the quadratic tensor action is identical to that of GR.
Figures
Caption
The fractional energy density $\Omega_{\mathrm{GW}}$ of SIGWs for a monochromatic curvature spectrum. Left: dependence on $\sigma$ with $\mu_s=0$. Right: dependence on $\mu_s$ in the limit $\sigma\rightarrow\infty$. The dashed curves correspond to $\sigma\to\infty$ in the left panel and $\mu_s=0$ in the right panel.Caption
The fractional energy density $\Omega_{\mathrm{GW}}$ of SIGWs for a monochromatic curvature spectrum. Left: dependence on $\sigma$ with $\mu_s=0$. Right: dependence on $\mu_s$ in the limit $\sigma\rightarrow\infty$. The dashed curves correspond to $\sigma\to\infty$ in the left panel and $\mu_s=0$ in the right panel.Caption
The fractional energy density $\Omega_{\mathrm{GW}}$ of SIGWs for a log-normal primordial spectrum with $\Delta_{\zeta}=0.1$. Left: dependence on $\sigma$ with $\mu_s=0$. Right: dependence on $\mu_s$ in the limit $\sigma\rightarrow\infty$. The dashed curves correspond to $\sigma\to\infty$ in the left panel and $\mu_s=0$ in the right panel.Caption
The fractional energy density $\Omega_{\mathrm{GW}}$ of SIGWs for a log-normal primordial spectrum with $\Delta_{\zeta}=0.1$. Left: dependence on $\sigma$ with $\mu_s=0$. Right: dependence on $\mu_s$ in the limit $\sigma\rightarrow\infty$. The dashed curves correspond to $\sigma\to\infty$ in the left panel and $\mu_s=0$ in the right panel.References
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