A microscopic model for inflation from supersymmetry breaking

Abstract We have proposed recently a framework for inflation driven by supersymmetry breaking with the inflaton being a superpartner of the goldstino, that avoids the main problems of supergravity inflation, allowing for: naturally small slow-roll parameters, small field initial conditions, absence...

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Main Authors: I. Antoniadis, A. Chatrabhuti, H. Isono, R. Knoops
Format: Article
Language:English
Published: SpringerOpen 2019-07-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-019-7141-5
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spelling doaj-148ee5416c34467fb0b00e2df0d7afb22020-11-25T03:09:18ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522019-07-0179712210.1140/epjc/s10052-019-7141-5A microscopic model for inflation from supersymmetry breakingI. Antoniadis0A. Chatrabhuti1H. Isono2R. Knoops3Laboratoire de Physique Théorique et Hautes Energies-LPTHE, Sorbonne Université, CNRSDepartment of Physics, Faculty of Science, Chulalongkorn UniversityDepartment of Physics, Faculty of Science, Chulalongkorn UniversityDepartment of Physics, Faculty of Science, Chulalongkorn UniversityAbstract We have proposed recently a framework for inflation driven by supersymmetry breaking with the inflaton being a superpartner of the goldstino, that avoids the main problems of supergravity inflation, allowing for: naturally small slow-roll parameters, small field initial conditions, absence of a (pseudo)scalar companion of the inflaton, and a nearby minimum with tuneable cosmological constant. It contains a chiral multiplet charged under a gauged R-symmetry which is restored at the maximum of the scalar potential with a plateau where inflation takes place. The effective field theory relies on two phenomenological parameters corresponding to corrections to the Kähler potential up to second order around the origin. The first guarantees the maximum at the origin and the second allows the tuning of the vacuum energy between the F- and D-term contributions. Here, we provide a microscopic model leading to the required effective theory. It is a Fayet–Iliopoulos model with two charged chiral multiplets under a second $$\mathrm{U}(1)$$ U(1) R-symmetry coupled to supergravity. In the Brout–Englert–Higgs phase of this $$\mathrm{U}(1)$$ U(1) , the gauge field becomes massive and can be integrated out in the limit of small supersymmetry breaking scale. In this work, we perform this integration and we show that there is a region of parameter space where the effective supergravity realises our proposal of small field inflation from supersymmetry breaking consistently with observations and with a minimum of tuneable energy that can describe the present phase of our Universe.http://link.springer.com/article/10.1140/epjc/s10052-019-7141-5
collection DOAJ
language English
format Article
sources DOAJ
author I. Antoniadis
A. Chatrabhuti
H. Isono
R. Knoops
spellingShingle I. Antoniadis
A. Chatrabhuti
H. Isono
R. Knoops
A microscopic model for inflation from supersymmetry breaking
European Physical Journal C: Particles and Fields
author_facet I. Antoniadis
A. Chatrabhuti
H. Isono
R. Knoops
author_sort I. Antoniadis
title A microscopic model for inflation from supersymmetry breaking
title_short A microscopic model for inflation from supersymmetry breaking
title_full A microscopic model for inflation from supersymmetry breaking
title_fullStr A microscopic model for inflation from supersymmetry breaking
title_full_unstemmed A microscopic model for inflation from supersymmetry breaking
title_sort microscopic model for inflation from supersymmetry breaking
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2019-07-01
description Abstract We have proposed recently a framework for inflation driven by supersymmetry breaking with the inflaton being a superpartner of the goldstino, that avoids the main problems of supergravity inflation, allowing for: naturally small slow-roll parameters, small field initial conditions, absence of a (pseudo)scalar companion of the inflaton, and a nearby minimum with tuneable cosmological constant. It contains a chiral multiplet charged under a gauged R-symmetry which is restored at the maximum of the scalar potential with a plateau where inflation takes place. The effective field theory relies on two phenomenological parameters corresponding to corrections to the Kähler potential up to second order around the origin. The first guarantees the maximum at the origin and the second allows the tuning of the vacuum energy between the F- and D-term contributions. Here, we provide a microscopic model leading to the required effective theory. It is a Fayet–Iliopoulos model with two charged chiral multiplets under a second $$\mathrm{U}(1)$$ U(1) R-symmetry coupled to supergravity. In the Brout–Englert–Higgs phase of this $$\mathrm{U}(1)$$ U(1) , the gauge field becomes massive and can be integrated out in the limit of small supersymmetry breaking scale. In this work, we perform this integration and we show that there is a region of parameter space where the effective supergravity realises our proposal of small field inflation from supersymmetry breaking consistently with observations and with a minimum of tuneable energy that can describe the present phase of our Universe.
url http://link.springer.com/article/10.1140/epjc/s10052-019-7141-5
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