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2005
DOI: 10.1088/1475-7516/2005/09/003
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A simple model for quintessential inflation

Abstract: We propose a simple toy model for quintessential inflation where a complex scalar field described by a lagrangian with a U (1) P Q symmetry spontaneously broken at a high energy scale and explicitly broken by instanton effects at a much lower energy can account for both the early inflationary phase and the recent accelerated expansion of the Universe. The real part of the complex field plays the role of the inflaton whereas the imaginary part, the "axion", is the quintessence field.

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Cited by 47 publications
(42 citation statements)
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References 44 publications
(53 reference statements)
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“…Similar to natural inflation [107], it has been proposed that the flatness of the quintessnce potential could be protected by the field being a pseudo-Nambu-Goldstone boson [108,109]. Additionally, it has been proposed that dark energy and inflation can both be driven by the same field [110][111][112][113][114][115][116][117][118] Quintessence models have a rich phenomenology; one of the more interesting phenomena is that-by suitably choosing the potential-the energy density in the quintessence field can be made to "track" the energy density in radiation/matter at early times and then grow to dominate the energy budget at late times [119][120][121][122][123][124][125][126]. The canonical example of a potential that produces this behavior is the Ratra-Peebles potential [67] V (φ) = M 4+n φ n , (2.4) where n > 0 is a constant.…”
Section: (23)mentioning
confidence: 99%
“…Similar to natural inflation [107], it has been proposed that the flatness of the quintessnce potential could be protected by the field being a pseudo-Nambu-Goldstone boson [108,109]. Additionally, it has been proposed that dark energy and inflation can both be driven by the same field [110][111][112][113][114][115][116][117][118] Quintessence models have a rich phenomenology; one of the more interesting phenomena is that-by suitably choosing the potential-the energy density in the quintessence field can be made to "track" the energy density in radiation/matter at early times and then grow to dominate the energy budget at late times [119][120][121][122][123][124][125][126]. The canonical example of a potential that produces this behavior is the Ratra-Peebles potential [67] V (φ) = M 4+n φ n , (2.4) where n > 0 is a constant.…”
Section: (23)mentioning
confidence: 99%
“…In this paper, we have studied the constraints on a simple model of quintessential inflation previously proposed by us [7] that arise from the WMAP3 CMB and SDSS LRG data. We find that the effective scale of symmetry breaking, f, must be larger than about 3 M Pl in order to satisfy the constraints on the scalar spectral index and the tensor-toscalar ratio from inflation at the 68% CL.…”
Section: Discussionmentioning
confidence: 99%
“…In Ref. [7], we introduced a simple, wellmotivated model that unifies these two fields into a single complex scalar field. We briefly review this model below.…”
Section: Introductionmentioning
confidence: 99%
“…When having N fields, our relations should of course be modified. In the simple case that the parameters of the N fields are identical, to convert the formulae in the text to the new case, we should make the following changes: To summarize, our purpose has been to give a step forward starting from the idea of Frieman and Rosenfeld [8] that fields in a potential may supply a unified explanation of inflation and dark energy. Our model contains two scalar fields, one complex and one real, and a potential that contains a non-symmetric part due to Planck-scale physics.…”
Section: Discussionmentioning
confidence: 99%