Implications of extreme flatness in a general f(R) theory

We discuss a modified gravity theory defined by f(R)=∑nlαnM2(1−n)Rn. We consider both finite and infinite number of terms in the series while requiring that the Einstein frame potential of the theory has a flat area around any of its stationary points. We show that the requirement of maximally flat...

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Main Authors: Michał Artymowski, Zygmunt Lalak, Marek Lewicki
Format: Article
Language:English
Published: Elsevier 2016-09-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269316303689
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spelling doaj-48cef6c1745c45bfbe37278154ec3c962020-11-24T22:21:38ZengElsevierPhysics Letters B0370-26931873-24452016-09-01760C43243710.1016/j.physletb.2016.07.027Implications of extreme flatness in a general f(R) theoryMichał Artymowski0Zygmunt Lalak1Marek Lewicki2Institute of Physics, Jagiellonian University, Łojasiewicza 11, 30-348 Kraków, PolandInstitute of Theoretical Physics, Faculty of Physics, University of Warsaw, ul. Pasteura 5, 02-093 Warsaw, PolandInstitute of Theoretical Physics, Faculty of Physics, University of Warsaw, ul. Pasteura 5, 02-093 Warsaw, PolandWe discuss a modified gravity theory defined by f(R)=∑nlαnM2(1−n)Rn. We consider both finite and infinite number of terms in the series while requiring that the Einstein frame potential of the theory has a flat area around any of its stationary points. We show that the requirement of maximally flat stationary point leads to the existence of the saddle point (local maximum) for even (odd) l. In both cases for l→∞ one obtains the Starobinsky model with small, exponentially suppressed corrections. Besides the GR minimum the Einstein frame potential has an anti de Sitter vacuum. However we argue that the GR vacuum is absolutely stable and AdS can be reached neither via classical evolution nor via quantum tunnelling. Our results show that a Starobinsky-like model is the only possible realisation of f(R) theory with an extremely flat area in the Einstein frame potential.http://www.sciencedirect.com/science/article/pii/S0370269316303689
collection DOAJ
language English
format Article
sources DOAJ
author Michał Artymowski
Zygmunt Lalak
Marek Lewicki
spellingShingle Michał Artymowski
Zygmunt Lalak
Marek Lewicki
Implications of extreme flatness in a general f(R) theory
Physics Letters B
author_facet Michał Artymowski
Zygmunt Lalak
Marek Lewicki
author_sort Michał Artymowski
title Implications of extreme flatness in a general f(R) theory
title_short Implications of extreme flatness in a general f(R) theory
title_full Implications of extreme flatness in a general f(R) theory
title_fullStr Implications of extreme flatness in a general f(R) theory
title_full_unstemmed Implications of extreme flatness in a general f(R) theory
title_sort implications of extreme flatness in a general f(r) theory
publisher Elsevier
series Physics Letters B
issn 0370-2693
1873-2445
publishDate 2016-09-01
description We discuss a modified gravity theory defined by f(R)=∑nlαnM2(1−n)Rn. We consider both finite and infinite number of terms in the series while requiring that the Einstein frame potential of the theory has a flat area around any of its stationary points. We show that the requirement of maximally flat stationary point leads to the existence of the saddle point (local maximum) for even (odd) l. In both cases for l→∞ one obtains the Starobinsky model with small, exponentially suppressed corrections. Besides the GR minimum the Einstein frame potential has an anti de Sitter vacuum. However we argue that the GR vacuum is absolutely stable and AdS can be reached neither via classical evolution nor via quantum tunnelling. Our results show that a Starobinsky-like model is the only possible realisation of f(R) theory with an extremely flat area in the Einstein frame potential.
url http://www.sciencedirect.com/science/article/pii/S0370269316303689
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AT zygmuntlalak implicationsofextremeflatnessinageneralfrtheory
AT mareklewicki implicationsofextremeflatnessinageneralfrtheory
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