Abstract

We propose a limited class of models, describing interacting chiral multiplets with a non-minimal coupling to a vector multiplet, in curved superspace of $N=1$ supergravity. Those models are suitable for the inflationary model building in supergravity with inflaton assigned to a massive vector multiplet and spontaneous SUSY breaking in Minkowski vacuum after inflation, for any values of the inflationary parameters $n_s$ and $r$, and any scale of SUSY breaking.

Highlights

  • Success of the inflationary scenario for early Universe is, on the one hand, due to overcoming the theoretical problems of the standard (Einstein-Friedmann) cosmology and, on the other hand, due to its remarkable agreement with the CMB observational data (COBE, WMAP, PLANCK)

  • There is the so-called η-problem caused by the presence of the exponential factor eK in the scalar potential of supergravity with chiral superfields, which generically prevents slow roll

  • There are problems with ensuring the inflaton scalar potential to be bounded from below, and with getting SUSY breaking in a Minkowski vacuum after inflation too

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Summary

Introduction

Success of the inflationary scenario for early Universe is, on the one hand, due to overcoming the theoretical problems (horizon, flatness, structure formation) of the standard (Einstein-Friedmann) cosmology and, on the other hand, due to its remarkable agreement with the CMB observational data (COBE, WMAP, PLANCK). The minimal inflationary models with a single inflaton chiral superfield, with or without SUSY breaking after inflation, are possible [11, 12, 13] but require tuning both Kahler potential and a superpotential. Another approach, based on the use of non-linear realizations of SUSY and nilpotent chiral superfields, was introduced to the supergravity-based inflationary model building in [14]. The supergravity inflationary models of [15] have the single-field scalar potential given by an arbitrary real function squared. As is clear from (9), the absence of ghosts requires J′′(C) > 0

Vacuum solution
Conclusion
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