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The Curvature Perturbation in the Axion-type Curvaton Model

Pravabati Chingangbam, Qing-Guo Huang

Abstract

We study the axion-type curvaton model, with emphasis on the large field regime where analytic results are very difficult to obtain. We evaluate the tensor-scalar ratio $r$ using WMAP normalization and the non-linearity parameters $f_{NL}$ and $g_{NL}$ by solving the equations numerically using the $δN$ formalism. We compare them with results for the curvaton with quadratic potential. We find that $r$ is much smaller for the axion-type case compared to the result from the quadratic potential, with the difference increasingly more pronounced at larger field values. $g_{NL}$ is found to be positive, unlike the quadratic case where it is negative, and the amplitude of $g_{NL}$ is much larger. Moreover, there is a nearly linear scaling between $g_{NL}$ and $f_{NL}$, with small deviation from linearity at large field values. The slope between $g_{NL}$ and $f_{NL}$ depends on the parameters characterizing the axion-type curvaton model. We further consider a mixed scenario where both the inflaton and the curvaton contribute to the primordial power spectrum and the non-Gaussianity parameters are found to be much larger than those in the case with quadratic potential.

The Curvature Perturbation in the Axion-type Curvaton Model

Abstract

We study the axion-type curvaton model, with emphasis on the large field regime where analytic results are very difficult to obtain. We evaluate the tensor-scalar ratio using WMAP normalization and the non-linearity parameters and by solving the equations numerically using the formalism. We compare them with results for the curvaton with quadratic potential. We find that is much smaller for the axion-type case compared to the result from the quadratic potential, with the difference increasingly more pronounced at larger field values. is found to be positive, unlike the quadratic case where it is negative, and the amplitude of is much larger. Moreover, there is a nearly linear scaling between and , with small deviation from linearity at large field values. The slope between and depends on the parameters characterizing the axion-type curvaton model. We further consider a mixed scenario where both the inflaton and the curvaton contribute to the primordial power spectrum and the non-Gaussianity parameters are found to be much larger than those in the case with quadratic potential.

Paper Structure

This paper contains 7 sections, 62 equations, 10 figures.

Figures (10)

  • Figure 1: The red (solid), blue (dotted) and green (dashed) lines correspond to the axion potential, quadratic potential and $\theta^2/2-\theta^4/24$ respectively.
  • Figure 2: The blue (dashed) line shows the exact value of $f_D$ computed numerically, whereas, the black (dotted) line shows to $f_D$ computed from the analytic approximation in Eq.(\ref{['afd']}), for the quadratic potential.
  • Figure 3: The red (solid) line shows $r$ for the cosine potential and the blue (dotted) line for the quadratic potential, respectively, for $\Gamma_{\sigma}/m = 10^{-4}$ and $10^{-5}$. $r$ is seen to decrease as $\Gamma_{\sigma}/m$ decreases.
  • Figure 4: Plot of $f_{NL}$. The red (solid), blue (dotted) and green (dashed) lines correspond to axion-type, quadratic and quadratic with $\sigma^4$ correction models, respectively.
  • Figure 5: Plot of $g_{NL}$. The red (solid), blue (dotted) and green (dashed) lines correspond to axion-type, quadratic and quadratic with $\sigma^4$ correction models, respectively.
  • ...and 5 more figures