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Natural supergravity inflation
We show that a single uncharged chiral superfield, canonically coupled to \mbox{$N=1$} supergravity with vanishing superpotential, naturally drives inflation in the early universe for a class of simple Kahler potentials. Inflation occurs due to the one-loop generation of a Kahler anomaly proportiona...
Autores principales: | , |
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Lenguaje: | eng |
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1993
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Acceso en línea: | https://dx.doi.org/10.1016/0370-2693(93)91823-6 http://cds.cern.ch/record/242132 |
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author | Lopes Cardoso, Gabriel Ovrut, Burt A. |
author_facet | Lopes Cardoso, Gabriel Ovrut, Burt A. |
author_sort | Lopes Cardoso, Gabriel |
collection | CERN |
description | We show that a single uncharged chiral superfield, canonically coupled to \mbox{$N=1$} supergravity with vanishing superpotential, naturally drives inflation in the early universe for a class of simple Kahler potentials. Inflation occurs due to the one-loop generation of a Kahler anomaly proportional to $\R^2$. The coefficient of this $\R^2$ term is of the correct magnitude to describe all aspects of an inflationary cosmology, including sufficient amplitude perturbations and reheating. Higher order terms proportional to $\R^n$ for $n \geq 3$ are naturally suppressed relative to the $\R^2$ term and, hence, do not destabilize the theory. |
id | cern-242132 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1993 |
record_format | invenio |
spelling | cern-2421322023-03-14T19:59:24Zdoi:10.1016/0370-2693(93)91823-6http://cds.cern.ch/record/242132engLopes Cardoso, GabrielOvrut, Burt A.Natural supergravity inflationParticle Physics - TheoryWe show that a single uncharged chiral superfield, canonically coupled to \mbox{$N=1$} supergravity with vanishing superpotential, naturally drives inflation in the early universe for a class of simple Kahler potentials. Inflation occurs due to the one-loop generation of a Kahler anomaly proportional to $\R^2$. The coefficient of this $\R^2$ term is of the correct magnitude to describe all aspects of an inflationary cosmology, including sufficient amplitude perturbations and reheating. Higher order terms proportional to $\R^n$ for $n \geq 3$ are naturally suppressed relative to the $\R^2$ term and, hence, do not destabilize the theory.We show that a single uncharged chiral superfield, canonically coupled to \mbox{$N=1$} supergravity with vanishing superpotential, naturally drives inflation in the early universe for a class of simple Kahler potentials. Inflation occurs due to the one-loop generation of a Kahler anomaly proportional to $\R~2$. The coefficient of this $\R~2$ term is of the correct magnitude to describe all aspects of an inflationary cosmology, including sufficient amplitude perturbations and reheating. Higher order terms proportional to $\R~n$ for $n \geq 3$ are naturally suppressed relative to the $\R~2$ term and, hence, do not destabilize the theory.We show that a single uncharged chiral superfield, canonically coupled to \mbox{$N=1$} supergravity with vanishing superpotential, naturally drives inflation in the early universe for a class of simple Kahler potentials. Inflation occurs due to the one-loop generation of a Kahler anomaly proportional to $\R~2$. The coefficient of this $\R~2$ term is of the correct magnitude to describe all aspects of an inflationary cosmology, including sufficient amplitude perturbations and reheating. Higher order terms proportional to $\R~n$ for $n \geq 3$ are naturally suppressed relative to the $\R~2$ term and, hence, do not destabilize the theory.We show that a single uncharged chiral superfield, canonically coupled to N = 1 supergravity with vanishing superpotential, naturally drives inflation in the early universe for a class of simple Kähler potentials. Inflation occurs due to the one-loop generation of a Kähler anomaly proportional to R 2 . The coefficient of this R 2 term is of the correct magnitude to describe all aspects of an inflationary cosmology, including sufficient amplitude perturbations and reheating. Higher order terms proportional to R n for n ⩾3 are naturally suppressed relative to the R 2 term and, hence, do not destabilize the theory.hep-th/9210114CERN-TH-6685-92UPR-0526-TCERN-TH-6685-92UPR-0526-Toai:cds.cern.ch:2421321993 |
spellingShingle | Particle Physics - Theory Lopes Cardoso, Gabriel Ovrut, Burt A. Natural supergravity inflation |
title | Natural supergravity inflation |
title_full | Natural supergravity inflation |
title_fullStr | Natural supergravity inflation |
title_full_unstemmed | Natural supergravity inflation |
title_short | Natural supergravity inflation |
title_sort | natural supergravity inflation |
topic | Particle Physics - Theory |
url | https://dx.doi.org/10.1016/0370-2693(93)91823-6 http://cds.cern.ch/record/242132 |
work_keys_str_mv | AT lopescardosogabriel naturalsupergravityinflation AT ovrutburta naturalsupergravityinflation |