Non-Gaussianity from axionic curvaton

被引:22
|
作者
Kawasaki, Masahiro [1 ,2 ]
Kobayashi, Takeshi [3 ,4 ]
Takahashi, Fuminobu [2 ,5 ]
机构
[1] Univ Tokyo, Inst Cosm Ray Res, Kashiwa, Chiba 2778582, Japan
[2] Univ Tokyo, Inst Phys & Math Universe, Kashiwa, Chiba 2778582, Japan
[3] Univ Toronto, Canadian Inst Theoret Astrophys, Toronto, ON M5S 3H8, Canada
[4] Perimeter Inst Theoret Phys, Waterloo, ON N2L 2Y5, Canada
[5] Tohoku Univ, Dept Phys, Sendai, Miyagi 9808578, Japan
关键词
axions; non-gaussianity; physics of the early universe; cosmological perturbation theory; HIGGS MASS; PERTURBATIONS; SUPERSYMMETRY; FIELDS;
D O I
10.1088/1475-7516/2013/03/016
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We study non-Gaussianity of density perturbations generated by an axionic curvaton, focusing on the case that the curvaton sits near the hilltop of the potential during inflation. Such hilltop curvatons can generate a red-tilted density perturbation spectrum without invoking large-field inflation. We show that, even when the curvaton dominates the Universe, the non-Gaussianity parameter f(NL) is positive and mildly increases towards the hilltop of the curvaton potential, and that f(NL) = O(10) is a general and robust prediction of such hilltop axionic curvatons. In particular, we find that the non-Gaussianity parameter is bounded as f(NL) less than or similar to 30 - 40 for a range of the scalar spectral index, n(s) = 0.94 - 0.99, and that f(NL) = 20 - 40 is realized for the curvaton mass m(sigma) = 10 - 10(6) GeV and the decay constant f = 10(12) - 10(17) GeV. One of the plausible candidates for the axionic curvaton is an imaginary component of a modulus field with mass of order 10 - 100 TeV and decay constant of 10(16-17) GeV. We also discuss extreme cases where the curvaton drives a second inflation and find that f(NL) is typically smaller compared to non-inflating cases.
引用
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页数:24
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