Abstract

We consider a possibility that the Higgs field in the Standard Model (SM) serves as an inflaton when its value is around the Planck scale. We assume that the SM is valid up to an ultraviolet cutoff scale \Lambda, which is slightly below the Planck scale, and that the Higgs potential becomes almost flat above \Lambda. Contrary to the ordinary Higgs inflation scenario, we do not assume the huge non-minimal coupling, of O(10^4), of the Higgs field to the Ricci scalar. We find that \Lambda must be less than 5*10^{17}GeV in order to explain the observed fluctuation of the cosmic microwave background, no matter how we extrapolate the Higgs potential above \Lambda. The scale 10^{17}GeV coincides with the perturbative string scale, which suggests that the SM is directly connected with the string theory. For this to be true, the top quark mass is restricted to around 171GeV, with which \Lambda can exceed 10^{17}GeV. As a concrete example of the potential above \Lambda, we propose a simple log type potential. The predictions of this specific model for the e-foldings N_*=50--60 are consistent with the current observation, namely, the scalar spectral index is n_s=0.977--0.983 and the tensor to scalar ratio 0<r<0.012--0.010. Other parameters, dn_s/dlnk, n_t, and their derivatives, are also consistent.

Highlights

  • It is more and more plausible that the particle discovered at the CERN Large Hadron Collider (LHC) [1,2] around 126 GeV is the Standard Model (SM) Higgs boson

  • The Higgs potential in the Standard Model (SM) can have a saddle point around 1017 GeV, and its height is suppressed because the Higgs quartic coupling becomes small

  • These facts suggest that the SM Higgs field may serve as an inflaton, without assuming the very large coupling to the Ricci scalar of order 104 which is necessary in the ordinary Higgs inflation scenario

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Summary

Introduction

It is more and more plausible that the particle discovered at the CERN Large Hadron Collider (LHC) [1,2] around 126 GeV is the Standard Model (SM) Higgs boson. The quadratically divergent bare Higgs mass is found to be suppressed too when the UV cutoff is 1017 GeV [4]; see Refs. This assumption is equivalent to the vanishing Higgs quartic coupling and its beta function at the Planck scale. The success of this prediction indicates that at least the top–Higgs sector of the SM remains unaltered up to a very high UV cutoff scale .1. In order to have an inflation consistent with the current observational data, we assume that the low-energy SM Higgs potential, depicted by the solid lines, is smoothly connected to an almost flat potential, depicted by the dot-dashed lines, around the UV cutoff scale .2.

Constraints on inflation models
SM Higgs potential
Higgs inflation?
Minimal Higgs inflation
Log-type potential
Summary and discussions
Full Text
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