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Low-scale Quintessential Inflation

In quintessential inflationary model, the same master field that drives inflation becomes, later on, the dynamical source of the (present) accelerated expansion. Quintessential inflationary models require a curvature scale at the end of inflation around $10^{-6}M_{\rm P}$ in order to explain the lar...

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Autor principal: Giovannini, Massimo
Lenguaje:eng
Publicado: 2003
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.67.123512
http://cds.cern.ch/record/603279
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author Giovannini, Massimo
author_facet Giovannini, Massimo
author_sort Giovannini, Massimo
collection CERN
description In quintessential inflationary model, the same master field that drives inflation becomes, later on, the dynamical source of the (present) accelerated expansion. Quintessential inflationary models require a curvature scale at the end of inflation around $10^{-6}M_{\rm P}$ in order to explain the large scale fluctuations observed in the microwave sky. If the curvature scale at the end of inflation is much smaller than $10^{-6}M_{\rm P}$, the large scale adiabatic mode may be produced thanks to the relaxation of a scalar degree of freedom, which will be generically denoted, according to the recent terminology, as the curvaton field. The production of the adiabatic mode is analysed in detail in the case of the minimal quintessential inflationary model originally proposed by Peebles and Vilenkin.
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institution Organización Europea para la Investigación Nuclear
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spelling cern-6032792019-09-30T06:29:59Zdoi:10.1103/PhysRevD.67.123512http://cds.cern.ch/record/603279engGiovannini, MassimoLow-scale Quintessential InflationParticle Physics - PhenomenologyIn quintessential inflationary model, the same master field that drives inflation becomes, later on, the dynamical source of the (present) accelerated expansion. Quintessential inflationary models require a curvature scale at the end of inflation around $10^{-6}M_{\rm P}$ in order to explain the large scale fluctuations observed in the microwave sky. If the curvature scale at the end of inflation is much smaller than $10^{-6}M_{\rm P}$, the large scale adiabatic mode may be produced thanks to the relaxation of a scalar degree of freedom, which will be generically denoted, according to the recent terminology, as the curvaton field. The production of the adiabatic mode is analysed in detail in the case of the minimal quintessential inflationary model originally proposed by Peebles and Vilenkin.hep-ph/0301264CERN-TH-2003-017oai:cds.cern.ch:6032792003-01-30
spellingShingle Particle Physics - Phenomenology
Giovannini, Massimo
Low-scale Quintessential Inflation
title Low-scale Quintessential Inflation
title_full Low-scale Quintessential Inflation
title_fullStr Low-scale Quintessential Inflation
title_full_unstemmed Low-scale Quintessential Inflation
title_short Low-scale Quintessential Inflation
title_sort low-scale quintessential inflation
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevD.67.123512
http://cds.cern.ch/record/603279
work_keys_str_mv AT giovanninimassimo lowscalequintessentialinflation