Abstract

Models of induced-gravity inflation are formulated within Supergravity employing as inflaton the Higgs field which leads to a spontaneous breaking of a U(1)_{B-L} symmetry at M_mathrm{GUT}=2cdot 10^{16}~{mathrm{GeV}}. We use a renormalizable superpotential, fixed by a U(1) R symmetry, and Kähler potentials which exhibit a quadratic non-minimal coupling to gravity with or without an independent kinetic mixing in the inflaton sector. In both cases we find inflationary solutions of Starobinsky type whereas in the latter case, others (more marginal) which resemble those of linear inflation arise too. In all cases the inflaton mass is predicted to be of the order of 10^{13}~{mathrm{GeV}}. Extending the superpotential of the model with suitable terms, we show how the MSSM mu parameter can be generated. Also, non-thermal leptogenesis can be successfully realized, provided that the gravitino is heavier than about 10~{mathrm{TeV}}.

Highlights

  • The idea of induced gravity (IG), according to which the Planck mass mP is generated [1,2] via the vacuum expectation value ( v.e.v) that a scalar field acquires at the end of a phase transition in the early universe, has recently attracted a fair amount of attention

  • With the ingredients above we can extract the part of the Einstein frame (EF) action within SUGRA related to the complex scalars zα = S, ̄ – denoted by the same superfield symbol

  • It is worthwhile to test the applicability of the framework above in the case of IG Higgs inflation (IGHI)

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Summary

Introduction

The idea of induced gravity (IG), according to which the (reduced) Planck mass mP is generated [1,2] via the vacuum expectation value ( v.e.v) that a scalar field acquires at the end of a phase transition in the early universe, has recently attracted a fair amount of attention This is because it may follow an inflationary stage driven by a Starobiskytype potential [3] in Supergravity (SUGRA) [4,5,6,7,8,9,10,11,12,13] and in non-Supersymmetric (SUSY) [14,15,16,17,18,19,20,21,22] settings, which turns out to be nicely compatible with the observational data [23].

Embedding induced-gravity HI in SUGRA
Set-up
From Einstein to Jordan frame
Induced-gravity requirement
Inflationary potential
Stability and loop-corrections
SUSY gauge coupling unification
General framework
Analytic results
Numerical results
A possible post-inflationary completion
Generating the μ parameter
Connection with the parameters of CMSSM
Non-thermal leptogenesis
Inflaton mass and decay
Lepton-number and gravitino abundances
Results
Conclusions
Full Text
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