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Curvaton dynamics

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Curvaton dynamics. / Dimopoulos, Konstantinos; Lazarides, George; Lyth, David H. et al.
In: Physical Review D, Vol. 68, No. 12, 123515, 15.12.2003.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Dimopoulos, K, Lazarides, G, Lyth, DH & Ruiz de Austri, R 2003, 'Curvaton dynamics', Physical Review D, vol. 68, no. 12, 123515. https://doi.org/10.1103/PhysRevD.68.123515

APA

Dimopoulos, K., Lazarides, G., Lyth, D. H., & Ruiz de Austri, R. (2003). Curvaton dynamics. Physical Review D, 68(12), Article 123515. https://doi.org/10.1103/PhysRevD.68.123515

Vancouver

Dimopoulos K, Lazarides G, Lyth DH, Ruiz de Austri R. Curvaton dynamics. Physical Review D. 2003 Dec 15;68(12):123515. doi: 10.1103/PhysRevD.68.123515

Author

Dimopoulos, Konstantinos ; Lazarides, George ; Lyth, David H. et al. / Curvaton dynamics. In: Physical Review D. 2003 ; Vol. 68, No. 12.

Bibtex

@article{eb5f17e343b047269392d93faa5c9f71,
title = "Curvaton dynamics",
abstract = "In contrast with the inflaton case, the curvature perturbations due to the curvaton field depend strongly on the evolution of the curvaton before its decay. We study in detail the dynamics of the curvaton evolution during and after inflation. We consider that the flatness of the curvaton potential may be affected by supergravity corrections, which introduce an effective mass proportional to the Hubble parameter. We also consider that the curvaton potential may be dominated by a quartic or by a non-renormalizable term. We find analytic solutions for the curvaton evolution for all these possibilities. In particular, we show that, in all the above cases, the curvaton density ratio with respect to the background density of the Universe decreases. Therefore, it is necessary that the curvaton decays only after its potential becomes dominated by the quadratic term, which results in (Hubble damped) sinusoidal oscillations. In the case when a non-renormalizable term dominates the potential, we find a possible non-oscillatory attractor solution that threatens to erase the curvature perturbation spectrum. Finally, we study the effects of thermal corrections to the curvaton potential and show that, if they ever dominate the effective mass, they lead to premature thermalization of the curvaton condensate. To avoid this danger, a stringent bound has to be imposed on the coupling of the curvaton to the thermal bath.",
author = "Konstantinos Dimopoulos and George Lazarides and Lyth, {David H.} and {Ruiz de Austri}, Roberto",
year = "2003",
month = dec,
day = "15",
doi = "10.1103/PhysRevD.68.123515",
language = "English",
volume = "68",
journal = "Physical Review D",
issn = "1550-7998",
publisher = "American Physical Society",
number = "12",

}

RIS

TY - JOUR

T1 - Curvaton dynamics

AU - Dimopoulos, Konstantinos

AU - Lazarides, George

AU - Lyth, David H.

AU - Ruiz de Austri, Roberto

PY - 2003/12/15

Y1 - 2003/12/15

N2 - In contrast with the inflaton case, the curvature perturbations due to the curvaton field depend strongly on the evolution of the curvaton before its decay. We study in detail the dynamics of the curvaton evolution during and after inflation. We consider that the flatness of the curvaton potential may be affected by supergravity corrections, which introduce an effective mass proportional to the Hubble parameter. We also consider that the curvaton potential may be dominated by a quartic or by a non-renormalizable term. We find analytic solutions for the curvaton evolution for all these possibilities. In particular, we show that, in all the above cases, the curvaton density ratio with respect to the background density of the Universe decreases. Therefore, it is necessary that the curvaton decays only after its potential becomes dominated by the quadratic term, which results in (Hubble damped) sinusoidal oscillations. In the case when a non-renormalizable term dominates the potential, we find a possible non-oscillatory attractor solution that threatens to erase the curvature perturbation spectrum. Finally, we study the effects of thermal corrections to the curvaton potential and show that, if they ever dominate the effective mass, they lead to premature thermalization of the curvaton condensate. To avoid this danger, a stringent bound has to be imposed on the coupling of the curvaton to the thermal bath.

AB - In contrast with the inflaton case, the curvature perturbations due to the curvaton field depend strongly on the evolution of the curvaton before its decay. We study in detail the dynamics of the curvaton evolution during and after inflation. We consider that the flatness of the curvaton potential may be affected by supergravity corrections, which introduce an effective mass proportional to the Hubble parameter. We also consider that the curvaton potential may be dominated by a quartic or by a non-renormalizable term. We find analytic solutions for the curvaton evolution for all these possibilities. In particular, we show that, in all the above cases, the curvaton density ratio with respect to the background density of the Universe decreases. Therefore, it is necessary that the curvaton decays only after its potential becomes dominated by the quadratic term, which results in (Hubble damped) sinusoidal oscillations. In the case when a non-renormalizable term dominates the potential, we find a possible non-oscillatory attractor solution that threatens to erase the curvature perturbation spectrum. Finally, we study the effects of thermal corrections to the curvaton potential and show that, if they ever dominate the effective mass, they lead to premature thermalization of the curvaton condensate. To avoid this danger, a stringent bound has to be imposed on the coupling of the curvaton to the thermal bath.

U2 - 10.1103/PhysRevD.68.123515

DO - 10.1103/PhysRevD.68.123515

M3 - Journal article

VL - 68

JO - Physical Review D

JF - Physical Review D

SN - 1550-7998

IS - 12

M1 - 123515

ER -