Kinetically modified non-minimal inflation with exponential frame function

Abstract We consider supersymmetric (SUSY) and non-SUSY models of chaotic inflation based on the $$\phi ^n$$ ϕ n potential with $$n=2$$ n = 2 or 4. We show that the coexistence of an exponential non-minimal coupling to gravity $$f_\mathcal{R}=\mathrm{e}^{c_\mathcal{R}\phi ^{p}}$$ f R = e c R ϕ p wit...

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Main Author: C. Pallis
Format: Article
Language:English
Published: SpringerOpen 2017-09-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-017-5165-2
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spelling doaj-9377cd9c812647a3a4359e5d60bbe9e02020-11-24T23:27:05ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522017-09-0177911710.1140/epjc/s10052-017-5165-2Kinetically modified non-minimal inflation with exponential frame functionC. Pallis0Department of Physics, University of CyprusAbstract We consider supersymmetric (SUSY) and non-SUSY models of chaotic inflation based on the $$\phi ^n$$ ϕ n potential with $$n=2$$ n = 2 or 4. We show that the coexistence of an exponential non-minimal coupling to gravity $$f_\mathcal{R}=\mathrm{e}^{c_\mathcal{R}\phi ^{p}}$$ f R = e c R ϕ p with a kinetic mixing of the form $$f_{\mathrm{K}}=c_{\mathrm{K}}f_\mathcal{R}^m$$ f K = c K f R m can accommodate inflationary observables favored by the Planck and Bicep2/Keck Array results for $$p=1$$ p = 1 and 2, $$1\le m\le 15$$ 1 ≤ m ≤ 15 and $$2.6\times 10^{-3}\le r_{\mathcal {R}\mathrm{K}}=c_\mathcal{R}/c_{\mathrm{K}}^{p/2}\le 1,$$ 2.6 × 10 - 3 ≤ r R K = c R / c K p / 2 ≤ 1 , where the upper limit is not imposed for $$p=1$$ p = 1 . Inflation is of hilltop type and it can be attained for subplanckian inflaton values with the corresponding effective theories retaining the perturbative unitarity up to the Planck scale. The supergravity embedding of these models is achieved employing two chiral gauge singlet supefields, a monomial superpotential and several (semi)logarithmic or semi-polynomial Kähler potentials.http://link.springer.com/article/10.1140/epjc/s10052-017-5165-2
collection DOAJ
language English
format Article
sources DOAJ
author C. Pallis
spellingShingle C. Pallis
Kinetically modified non-minimal inflation with exponential frame function
European Physical Journal C: Particles and Fields
author_facet C. Pallis
author_sort C. Pallis
title Kinetically modified non-minimal inflation with exponential frame function
title_short Kinetically modified non-minimal inflation with exponential frame function
title_full Kinetically modified non-minimal inflation with exponential frame function
title_fullStr Kinetically modified non-minimal inflation with exponential frame function
title_full_unstemmed Kinetically modified non-minimal inflation with exponential frame function
title_sort kinetically modified non-minimal inflation with exponential frame function
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2017-09-01
description Abstract We consider supersymmetric (SUSY) and non-SUSY models of chaotic inflation based on the $$\phi ^n$$ ϕ n potential with $$n=2$$ n = 2 or 4. We show that the coexistence of an exponential non-minimal coupling to gravity $$f_\mathcal{R}=\mathrm{e}^{c_\mathcal{R}\phi ^{p}}$$ f R = e c R ϕ p with a kinetic mixing of the form $$f_{\mathrm{K}}=c_{\mathrm{K}}f_\mathcal{R}^m$$ f K = c K f R m can accommodate inflationary observables favored by the Planck and Bicep2/Keck Array results for $$p=1$$ p = 1 and 2, $$1\le m\le 15$$ 1 ≤ m ≤ 15 and $$2.6\times 10^{-3}\le r_{\mathcal {R}\mathrm{K}}=c_\mathcal{R}/c_{\mathrm{K}}^{p/2}\le 1,$$ 2.6 × 10 - 3 ≤ r R K = c R / c K p / 2 ≤ 1 , where the upper limit is not imposed for $$p=1$$ p = 1 . Inflation is of hilltop type and it can be attained for subplanckian inflaton values with the corresponding effective theories retaining the perturbative unitarity up to the Planck scale. The supergravity embedding of these models is achieved employing two chiral gauge singlet supefields, a monomial superpotential and several (semi)logarithmic or semi-polynomial Kähler potentials.
url http://link.springer.com/article/10.1140/epjc/s10052-017-5165-2
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