Abstract

We consider a simple inflation model with a complex scalar field coupled to gravity non-minimally. Both the modulus and the angular directions of the complex scalar are slowly rolling, leading to two-field inflation. The modulus direction becomes flat due to the non-minimal coupling, and the angular direction becomes a pseudo-Goldstone boson from a small breaking of the global U(1) symmetry. We show that large non-Gaussianity can be produced during slow-roll inflation under a reasonable assumption on the initial condition of the angular direction. This scenario may be realized in particle physics models such as the Standard Model with two Higgs doublets.

Highlights

  • Cosmic inflation [1] has been the cornerstone beyond the standard big bang cosmology

  • We have studied a simple multi-field inflation model by introducing a complex scalar field with non-minimal coupling to gravity

  • We have considered the general action for the complex scalar field with dimension-4 interactions in the potential

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Summary

Introduction

Cosmic inflation [1] has been the cornerstone beyond the standard big bang cosmology It makes the present observable universe homogeneous and isotropic on large scales and gives rise to the primordial perturbations [2]. The potential of the modulus of the complex scalar becomes flat at large field value due to the non-minimal coupling. This is comparable to √a similar observation in Higgs inflation that the gauge boson mass during inflation is of O(1/ ξ), which is identified with the ultraviolet cutoff during inflation [14] This is a simple Lagrangian [19] which has been studied in models motivated from string theory: it includes a non-canonical kinetic term with e2b(φ) ≡ 1 − e−2φ/ 6 ,. As will be shown later, the above product form of the potential makes it easy to study two-field inflation, for the background evolution and for the explicit computations of the perturbations using the δN formalism

Slow-roll parameters
Number of e-folds
Perturbations during slow-roll inflation
Linear perturbation
Non-Gaussianity
Conclusions
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