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Vector curvaton with varying kinetic function

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Vector curvaton with varying kinetic function. / Dimopoulos, Konstantinos; Karciauskas, Mindaugas; Wagstaff, Jacques M.
In: Physical Review D, Vol. 81, No. 2, 29.01.2010, p. 023522.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Dimopoulos, K, Karciauskas, M & Wagstaff, JM 2010, 'Vector curvaton with varying kinetic function', Physical Review D, vol. 81, no. 2, pp. 023522. https://doi.org/10.1103/PhysRevD.81.023522

APA

Dimopoulos, K., Karciauskas, M., & Wagstaff, J. M. (2010). Vector curvaton with varying kinetic function. Physical Review D, 81(2), 023522. https://doi.org/10.1103/PhysRevD.81.023522

Vancouver

Dimopoulos K, Karciauskas M, Wagstaff JM. Vector curvaton with varying kinetic function. Physical Review D. 2010 Jan 29;81(2):023522. doi: 10.1103/PhysRevD.81.023522

Author

Dimopoulos, Konstantinos ; Karciauskas, Mindaugas ; Wagstaff, Jacques M. / Vector curvaton with varying kinetic function. In: Physical Review D. 2010 ; Vol. 81, No. 2. pp. 023522.

Bibtex

@article{40b8852775ae4798befaef993337cf56,
title = "Vector curvaton with varying kinetic function",
abstract = "A new model realization of the vector curvaton paradigm is presented and analyzed. The model consists of a single massive Abelian vector field, with a Maxwell-type kinetic term. By assuming that the kinetic function and the mass of the vector field are appropriately varying during inflation, it is shown that a scaleinvariant spectrum of superhorizon perturbations can be generated. These perturbations can contribute to the curvature perturbation of the Universe. If the vector field remains light at the end of inflation it is found that it can generate substantial statistical anisotropy in the spectrum and bispectrum of the curvature perturbation. In this case the non-Gaussianity in the curvature perturbation is predominantly anisotropic, which will be a testable prediction in the near future. If, on the other hand, the vector field is heavy at the end of inflation then it is demonstrated that particle production is approximately isotropic and the vector field alone can give rise to the curvature perturbation, without directly involving any fundamental scalar field. The parameter space for both possibilities is shown to be substantial. Finally, toy models are presented which show that the desired variation of the mass and kinetic function of the vector field can be realistically obtained, without unnatural tunings, in the context of supergravity or superstrings.",
keywords = "cosmology, cosmic inflation, curvature perturbations, vector fields",
author = "Konstantinos Dimopoulos and Mindaugas Karciauskas and Wagstaff, {Jacques M.}",
year = "2010",
month = jan,
day = "29",
doi = "10.1103/PhysRevD.81.023522",
language = "English",
volume = "81",
pages = "023522",
journal = "Physical Review D",
issn = "1550-7998",
publisher = "American Physical Society",
number = "2",

}

RIS

TY - JOUR

T1 - Vector curvaton with varying kinetic function

AU - Dimopoulos, Konstantinos

AU - Karciauskas, Mindaugas

AU - Wagstaff, Jacques M.

PY - 2010/1/29

Y1 - 2010/1/29

N2 - A new model realization of the vector curvaton paradigm is presented and analyzed. The model consists of a single massive Abelian vector field, with a Maxwell-type kinetic term. By assuming that the kinetic function and the mass of the vector field are appropriately varying during inflation, it is shown that a scaleinvariant spectrum of superhorizon perturbations can be generated. These perturbations can contribute to the curvature perturbation of the Universe. If the vector field remains light at the end of inflation it is found that it can generate substantial statistical anisotropy in the spectrum and bispectrum of the curvature perturbation. In this case the non-Gaussianity in the curvature perturbation is predominantly anisotropic, which will be a testable prediction in the near future. If, on the other hand, the vector field is heavy at the end of inflation then it is demonstrated that particle production is approximately isotropic and the vector field alone can give rise to the curvature perturbation, without directly involving any fundamental scalar field. The parameter space for both possibilities is shown to be substantial. Finally, toy models are presented which show that the desired variation of the mass and kinetic function of the vector field can be realistically obtained, without unnatural tunings, in the context of supergravity or superstrings.

AB - A new model realization of the vector curvaton paradigm is presented and analyzed. The model consists of a single massive Abelian vector field, with a Maxwell-type kinetic term. By assuming that the kinetic function and the mass of the vector field are appropriately varying during inflation, it is shown that a scaleinvariant spectrum of superhorizon perturbations can be generated. These perturbations can contribute to the curvature perturbation of the Universe. If the vector field remains light at the end of inflation it is found that it can generate substantial statistical anisotropy in the spectrum and bispectrum of the curvature perturbation. In this case the non-Gaussianity in the curvature perturbation is predominantly anisotropic, which will be a testable prediction in the near future. If, on the other hand, the vector field is heavy at the end of inflation then it is demonstrated that particle production is approximately isotropic and the vector field alone can give rise to the curvature perturbation, without directly involving any fundamental scalar field. The parameter space for both possibilities is shown to be substantial. Finally, toy models are presented which show that the desired variation of the mass and kinetic function of the vector field can be realistically obtained, without unnatural tunings, in the context of supergravity or superstrings.

KW - cosmology

KW - cosmic inflation

KW - curvature perturbations

KW - vector fields

UR - http://www.scopus.com/inward/record.url?scp=77649225592&partnerID=8YFLogxK

U2 - 10.1103/PhysRevD.81.023522

DO - 10.1103/PhysRevD.81.023522

M3 - Journal article

VL - 81

SP - 023522

JO - Physical Review D

JF - Physical Review D

SN - 1550-7998

IS - 2

ER -