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Reconstruction of potentials of the hybrid inflation in the light of primordial black hole formation

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 Publication date 2021
  fields Physics
and research's language is English




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The large enhancement of the primordial power spectrum of the curvature perturbation can seed the formation of primordial black hole, that can play as a dark matter component in the Universe. In multi-filed inflation models, the curved trajectory of the scalar fields in the field space can generate a peak in the power spectrum on small scales due to the existence of the isocurvature perturbation. Here we show that a potential can be reconstructed from a given power spectrum, which is made of a scale-invariant one on large scales and the other function with a peak on small scales. In multi-field inflation models the reconstructed potential may not be unique and we can find different potentials from a given power spectrum.



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Within the framework of Galileon inflation with quartic and natural potentials, we investigate generation of the primordial black holes (PBHs) and induced gravitational waves (GWs). In this setup, we consider a Galileon function as $G(phi)=g_I(phi)big(1+g_{II}(phi)big)$ and show that in the presence of first term $g_I(phi)$ both quartic and natural potentials, in contrast to the standard model of inflation, can be consistent, with the 68% CL of Planck observations. Besides, the second term $g_{II}(phi)$ can cause a significant enhancement in the primordial curvature perturbations at the small scales which results the PBHs formation. For the both potentials, we obtain an enhancement in the scalar power spectrum at the scales $ksim10^{12}~rm Mpc^{-1}$, $10^{8}~rm Mpc^{-1}$, and $10^{5}~rm Mpc^{-1}$, which causes PBHs production in mass scales around $10^{-13}M_{odot}$, $10^{-5}M_{odot}$, and $10 M_{odot}$, respectively. Observational constraints confirm that PBHs with a mass scale of $10^{-13}M_{odot}$ can constitute the total of dark matter in the universe. Furthermore, we estimate the energy density parameter of induced GWs which can be examined by the observation. Also we conclude that it can be parametrized as a power-law function $Omega_{rm GW}sim (f/f_c)^n$, where the power index equals $n=3-2/ln(f_c/f)$ in the infrared limit $fll f_{c}$.
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