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No-Scale Inflation

Supersymmetry is the most natural framework for physics above the TeV scale, and the corresponding framework for early-Universe cosmology, including inflation, is supergravity. No-scale supergravity emerges from generic string compactifications and yields a non-negative potential, and is therefore a...

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Detalles Bibliográficos
Autores principales: Ellis, John, Garcia, Marcos A. G., Nanopoulos, Dimitri V., Olive, Keith A.
Lenguaje:eng
Publicado: 2015
Materias:
Acceso en línea:https://dx.doi.org/10.1088/0264-9381/33/9/094001
http://cds.cern.ch/record/2032906
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author Ellis, John
Garcia, Marcos A. G.
Nanopoulos, Dimitri V.
Olive, Keith A.
author_facet Ellis, John
Garcia, Marcos A. G.
Nanopoulos, Dimitri V.
Olive, Keith A.
author_sort Ellis, John
collection CERN
description Supersymmetry is the most natural framework for physics above the TeV scale, and the corresponding framework for early-Universe cosmology, including inflation, is supergravity. No-scale supergravity emerges from generic string compactifications and yields a non-negative potential, and is therefore a plausible framework for constructing models of inflation. No-scale inflation yields naturally predictions similar to those of the Starobinsky model based on $R + R^2$ gravity, with a tilted spectrum of scalar perturbations: $n_s \sim 0.96$, and small values of the tensor-to-scalar perturbation ratio $r < 0.1$, as favoured by Planck and other data on the cosmic microwave background (CMB). Detailed measurements of the CMB may provide insights into the embedding of inflation within string theory as well as its links to collider physics.
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spelling cern-20329062021-05-03T20:05:35Zdoi:10.1088/0264-9381/33/9/094001http://cds.cern.ch/record/2032906engEllis, JohnGarcia, Marcos A. G.Nanopoulos, Dimitri V.Olive, Keith A.No-Scale InflationParticle Physics - PhenomenologySupersymmetry is the most natural framework for physics above the TeV scale, and the corresponding framework for early-Universe cosmology, including inflation, is supergravity. No-scale supergravity emerges from generic string compactifications and yields a non-negative potential, and is therefore a plausible framework for constructing models of inflation. No-scale inflation yields naturally predictions similar to those of the Starobinsky model based on $R + R^2$ gravity, with a tilted spectrum of scalar perturbations: $n_s \sim 0.96$, and small values of the tensor-to-scalar perturbation ratio $r < 0.1$, as favoured by Planck and other data on the cosmic microwave background (CMB). Detailed measurements of the CMB may provide insights into the embedding of inflation within string theory as well as its links to collider physics.Supersymmetry is the most natural framework for physics above the TeV scale, and the corresponding framework for early-Universe cosmology, including inflation, is supergravity. No-scale supergravity emerges from generic string compactifications and yields a non-negative potential, and is therefore a plausible framework for constructing models of inflation. No-scale inflation yields naturally predictions similar to those of the Starobinsky model based on $R+{R}^{2}$ gravity, with a tilted spectrum of scalar perturbations: ${n}_{s}\sim 0.96$, and small values of the tensor-to-scalar perturbation ratio $r\lt 0.1$, as favoured by Planck and other data on the cosmic microwave background (CMB). Detailed measurements of the CMB may provide insights into the embedding of inflation within string theory as well as its links to collider physics.Supersymmetry is the most natural framework for physics above the TeV scale, and the corresponding framework for early-Universe cosmology, including inflation, is supergravity. No-scale supergravity emerges from generic string compactifications and yields a non-negative potential, and is therefore a plausible framework for constructing models of inflation. No-scale inflation yields naturally predictions similar to those of the Starobinsky model based on $R + R^2$ gravity, with a tilted spectrum of scalar perturbations: $n_s \sim 0.96$, and small values of the tensor-to-scalar perturbation ratio $r < 0.1$, as favoured by Planck and other data on the cosmic microwave background (CMB). Detailed measurements of the CMB may provide insights into the embedding of inflation within string theory as well as its links to collider physics.KCL-PH-TH-2015-28LCTS-2015-20CERN-PH-TH-2015-144ACT-05-15UMN-TH-3442-15FTPI-MINN-15-32arXiv:1507.02308MI-TH-1521KCL-PH-TH-2015-28LCTS-2015-20CERN-PH-TH-2015-144ACT-05-15MI-TH-1521UMN-TH-3442-15FTPI-MINN-15-32oai:cds.cern.ch:20329062015-07-08
spellingShingle Particle Physics - Phenomenology
Ellis, John
Garcia, Marcos A. G.
Nanopoulos, Dimitri V.
Olive, Keith A.
No-Scale Inflation
title No-Scale Inflation
title_full No-Scale Inflation
title_fullStr No-Scale Inflation
title_full_unstemmed No-Scale Inflation
title_short No-Scale Inflation
title_sort no-scale inflation
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1088/0264-9381/33/9/094001
http://cds.cern.ch/record/2032906
work_keys_str_mv AT ellisjohn noscaleinflation
AT garciamarcosag noscaleinflation
AT nanopoulosdimitriv noscaleinflation
AT olivekeitha noscaleinflation