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Multi-Natural Inflation

Michael Czerny, Fuminobu Takahashi

Abstract

We propose a multi-natural inflation model in which the single-field inflaton potential consists of two or more sinusoidal potentials that are comparable in size, but have different periodicity with a possible non-zero relative phase. The model is versatile enough to realize both large-field and small-field inflation. We show that, in a model with two sinusoidal potentials, the predicted values of the spectral index and tensor-to-scalar ratio lie within the $1σ$ region of the Planck data. In particular, there is no lower bound on the decay constants in contrast to the original natural inflation. We also show that, in a certain limit, multi-natural inflation can be approximated by a hilltop quartic inflation model.

Multi-Natural Inflation

Abstract

We propose a multi-natural inflation model in which the single-field inflaton potential consists of two or more sinusoidal potentials that are comparable in size, but have different periodicity with a possible non-zero relative phase. The model is versatile enough to realize both large-field and small-field inflation. We show that, in a model with two sinusoidal potentials, the predicted values of the spectral index and tensor-to-scalar ratio lie within the region of the Planck data. In particular, there is no lower bound on the decay constants in contrast to the original natural inflation. We also show that, in a certain limit, multi-natural inflation can be approximated by a hilltop quartic inflation model.

Paper Structure

This paper contains 5 sections, 24 equations, 4 figures.

Figures (4)

  • Figure 1: Left: the prediction of $(n_s, r)$ of multi-natural inflation for three different values of $\Lambda_2^4$. Solid (dashed) lines correspond to the e-folding number $N=60$ ($N=50$). Right: the corresponding inflaton potentials. The red dots represent the position at horizon crossing at $N= 60$ for the case of $B=0.40$.
  • Figure 2: Same as Fig. \ref{['fig:nsr1']} but for different values of the relative phase $\theta$.
  • Figure 3: Behavior of $n_s$ (left) and $r$ (right) as a function of $f$. The shaded regions in the left figure correspond to 1 and 2$\sigma$ allowed regions for $n_s$ from Planck data. The shaded region on the right corresponds to the 95% CL for $r$ ($r < 0.11$).
  • Figure 4: Planck normalized values for $\Lambda$ (left) and $m_\phi$ (right) as a function of $f$.