Implementing quadratic supergravity inflation
We study inflation driven by a slow-rolling inflaton field, characterised by a quadratic potential, and incorporating radiative corrections within the context of supergravity. In this model the energy scale of inflation is not overly constrained by the requirement of generating the observed level of...
Main Authors: | , , |
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Format: | Journal article |
Language: | English |
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1999
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_version_ | 1797077214401921024 |
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author | German, G Ross, G Sarkar, S |
author_facet | German, G Ross, G Sarkar, S |
author_sort | German, G |
collection | OXFORD |
description | We study inflation driven by a slow-rolling inflaton field, characterised by a quadratic potential, and incorporating radiative corrections within the context of supergravity. In this model the energy scale of inflation is not overly constrained by the requirement of generating the observed level of density fluctuations and can have a physically interesting value, e.g. the supersymmetry breaking scale of $10^{10}$ GeV or the electroweak scale of $10^3$ GeV. In this mass range the inflaton is light enough to be confined at the origin by thermal effects, naturally generating the initial conditions for a (last) stage of inflation of the new inflationary type. |
first_indexed | 2024-03-07T00:14:42Z |
format | Journal article |
id | oxford-uuid:7a687835-e1a1-4ce2-afc4-dc732e6e3eba |
institution | University of Oxford |
language | English |
last_indexed | 2024-03-07T00:14:42Z |
publishDate | 1999 |
record_format | dspace |
spelling | oxford-uuid:7a687835-e1a1-4ce2-afc4-dc732e6e3eba2022-03-26T20:43:57ZImplementing quadratic supergravity inflationJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:7a687835-e1a1-4ce2-afc4-dc732e6e3ebaEnglishSymplectic Elements at Oxford1999German, GRoss, GSarkar, SWe study inflation driven by a slow-rolling inflaton field, characterised by a quadratic potential, and incorporating radiative corrections within the context of supergravity. In this model the energy scale of inflation is not overly constrained by the requirement of generating the observed level of density fluctuations and can have a physically interesting value, e.g. the supersymmetry breaking scale of $10^{10}$ GeV or the electroweak scale of $10^3$ GeV. In this mass range the inflaton is light enough to be confined at the origin by thermal effects, naturally generating the initial conditions for a (last) stage of inflation of the new inflationary type. |
spellingShingle | German, G Ross, G Sarkar, S Implementing quadratic supergravity inflation |
title | Implementing quadratic supergravity inflation |
title_full | Implementing quadratic supergravity inflation |
title_fullStr | Implementing quadratic supergravity inflation |
title_full_unstemmed | Implementing quadratic supergravity inflation |
title_short | Implementing quadratic supergravity inflation |
title_sort | implementing quadratic supergravity inflation |
work_keys_str_mv | AT germang implementingquadraticsupergravityinflation AT rossg implementingquadraticsupergravityinflation AT sarkars implementingquadraticsupergravityinflation |