New models of Quintessential Inflation featuring plateau and hilltop potentials

Fuente: arXiv
Saved in:
Bibliographic Details
Main Authors: Mishra, Swagat S., Sahni, Varun
Format: Preprint
Published: 2024
Subjects:
Online Access:
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1866911772555870208
author Mishra, Swagat S.
Sahni, Varun
author_facet Mishra, Swagat S.
Sahni, Varun
contents We introduce a new class of hilltop and plateau potentials which can successfully unify inflation and dark energy resulting in Quintessential Inflation (QI). Interestingly these new potentials are related through an inverse transformation. Namely, if $V(ϕ) = V_0 \, v(ϕ)$ is a plateau potential then the inverse potential $V(ϕ) = V_0 \, \left[v(ϕ)\right]^{-1}$ describes hilltop QI. A simple example is provided by the KKLT-inspired potential $v(ϕ) = \left\lbrack \frac{M^{2n} + ϕ^{2n}}{N^{2n} + ϕ^{2n}}\right\rbrack \,$. When $M/N \ll 1$ this potential describes plateau QI, while its inverse, $\left[v(ϕ)\right]^{-1}$ describes hilltop QI. Other simple models of QI arise for the class of potentials $V(ϕ) \sim \exp\left\lbrack\mp f(ϕ)\right\rbrack$, where the $-$ ($+$) sign is associated with a plateau (hilltop). A key feature of this new class of QI models is the near absence of small parameters which are usually associated with the presence of dark energy. A forecast for the gravitational wave background generated in these models is provided.
format Preprint
id arxiv_https___arxiv_org_abs_2402_04316
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle New models of Quintessential Inflation featuring plateau and hilltop potentials
Mishra, Swagat S.
Sahni, Varun
Cosmology and Nongalactic Astrophysics
General Relativity and Quantum Cosmology
High Energy Physics - Phenomenology
High Energy Physics - Theory
We introduce a new class of hilltop and plateau potentials which can successfully unify inflation and dark energy resulting in Quintessential Inflation (QI). Interestingly these new potentials are related through an inverse transformation. Namely, if $V(ϕ) = V_0 \, v(ϕ)$ is a plateau potential then the inverse potential $V(ϕ) = V_0 \, \left[v(ϕ)\right]^{-1}$ describes hilltop QI. A simple example is provided by the KKLT-inspired potential $v(ϕ) = \left\lbrack \frac{M^{2n} + ϕ^{2n}}{N^{2n} + ϕ^{2n}}\right\rbrack \,$. When $M/N \ll 1$ this potential describes plateau QI, while its inverse, $\left[v(ϕ)\right]^{-1}$ describes hilltop QI. Other simple models of QI arise for the class of potentials $V(ϕ) \sim \exp\left\lbrack\mp f(ϕ)\right\rbrack$, where the $-$ ($+$) sign is associated with a plateau (hilltop). A key feature of this new class of QI models is the near absence of small parameters which are usually associated with the presence of dark energy. A forecast for the gravitational wave background generated in these models is provided.
title New models of Quintessential Inflation featuring plateau and hilltop potentials
topic Cosmology and Nongalactic Astrophysics
General Relativity and Quantum Cosmology
High Energy Physics - Phenomenology
High Energy Physics - Theory
url https://arxiv.org/abs/2402.04316