Abstract

We study the details of eternal inflation in the presence of a spectator Higgs field within the framework of the minimal Standard Model. We have recently shown that in the presence of scalar field(s) which allow inflation only within a finite domain of field values, the universe reaches a steady state where the normalized distribution for the field(s) converges to a steady state distribution [1]. In this paper, we analyze this eternal inflation scenario with the renormalized Standard Model Higgs potential, since it also allows inflation in a finite domain, but turns over at high scales due to the running of the self-coupling, marking an exit from inflation. We compute the full steady state distribution for the Higgs using an integral evolution technique that we formulated in [1] and the fractal dimension of the universe. We then obtain a bound on the inflationary Hubble scale in order to have a large observable universe contained within the instability scale of $H\lesssim\mathcal{O}(10^9)$GeV depending on the top mass. Upon reheating of the universe, thermal fluctuations in the Higgs field could potentially pose another problem; however, we compute the rate of thermal bubble production and find that the probability of tunneling in the post-inflationary era is negligibly small even for very high reheat temperatures.

Highlights

  • The discovery of the Higgs boson [1], which is required to maintain unitarity of W, Z boson scattering, completes the Standard Model (SM) of elementary particles

  • We know that the theory does violate unitarity at the Planck scale, but one wonders at what scale, if any, new physics enters before the Planck scale

  • Since the SM Higgs field develops an instability at high field values, thereby allowing an inflationary phase only in a finite domain, the Universe gets to an eternally inflating steady state in which any initial transient behavior washes out, and all interesting quantities like average volumes of regions, fractal dimensions, etc., are independent of the number of e-foldings provided in the final stages of slow-roll inflation

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Summary

INTRODUCTION

The discovery of the Higgs boson [1], which is required to maintain unitarity of W, Z boson scattering, completes the Standard Model (SM) of elementary particles. Apart from pointing out subtleties and assumptions made in this subject in the literature, our primary objective is twofold: first, to compute the abovementioned statistical quantities for the eternally inflating universe in the presence of the SM Higgs For this we make use of an integral (kernel) evolution technique [29] for the distribution of the Higgs (radial degree of freedom in a 4D Euclidean field space). In the Appendix we include the relevant SM beta functions

EVOLUTION OF RADIAL FIELD AND STEADY STATE
Kernel for radial field
Gaussian approximation and its limitations
Comparisons
ANALYSIS WITH THE STANDARD MODEL HIGGS
Tunneling probability at finite temperature
SUMMARY
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