Planck constraints on single-field inflation

We place observational constraints on slow-variation single-field inflationary models by carrying out the cosmological Monte Carlo simulation with the recent data of Planck combined with the WMAP large-angle polarization, baryon acoustic oscillations, and Atacama Cosmology Telescope/South Pole Teles...

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Veröffentlicht in:Physical review. D, Particles, fields, gravitation, and cosmology Particles, fields, gravitation, and cosmology, 2013-07, Vol.88 (2), Article 023529
Hauptverfasser: Tsujikawa, Shinji, Ohashi, Junko, Kuroyanagi, Sachiko, De Felice, Antonio
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Sprache:eng
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Zusammenfassung:We place observational constraints on slow-variation single-field inflationary models by carrying out the cosmological Monte Carlo simulation with the recent data of Planck combined with the WMAP large-angle polarization, baryon acoustic oscillations, and Atacama Cosmology Telescope/South Pole Telescope temperature data. Our analysis covers a wide variety of models with second-order equations of motion, including potential-driven slow-roll inflation, nonminimally coupled models, running kinetic couplings, Brans-Dicke theories, potential-driven Galileon inflation, field-derivative couplings to the Einstein tensor, and k-inflation. In the presence of running kinetic exponential couplings, covariant Galileon terms, and field-derivative couplings, the tensor-to-scalar ratio of the self-coupling potential V([varphi]) = [lambda][varphi] super(4)/4 gets smaller relative to that in standard slow-roll inflation, but the models lie outside the 1[sigma] observational contour. We also show that k-inflation models can be tightly constrained by adding the bounds from the scalar non-Gaussianities. The small-field inflationary models with asymptotic flat Einstein-frame potentials in the regime [varphi] >> M sub(pl) generally fit the data very well. These include the models such as Kahler-moduli inflation, nonminimally coupled Higgs inflation, and inflation in Brans-Dicke theories in the presence of the potential V([varphi]) = 3M super(2)([varphi] - M sub(pl)) super(2)/4 with the Brans-Dicke parameter omega sub(BD) [
ISSN:1550-7998
1550-2368
DOI:10.1103/PhysRevD.88.023529