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arXiv 0904.2649hep-thgr-qchep-ph
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多场暴胀结束时产生的非高斯性的几何描述

A geometric description of the non-Gaussianity generated at the end of multi-field inflation

Qing-Guo Huang

摘要:

本文主要研究了多场暴胀(如多桥暴胀)结束时产生的曲率扰动。由于曲率扰动是在超视界尺度上产生的,所以双谱和三谱具有局部形状。双谱的大小用$f_{NL}$表示,三谱的大小用两个参数$τ_{NL}$和$g_{NL}$表示。为了简单起见,假设暴胀子的轨道在场空间中是一条直线,那么在暴胀过程中,熵扰动对曲率扰动没有贡献。只要背景暴胀子路径不与暴胀结束的超曲面正交,熵扰动就能对暴胀结束时的曲率扰动作出贡献,并产生大的局域型非高斯性.有趣的是,非高斯参数完全由暴胀结束时超曲面的几何性质决定。例如,$f_{NL}$与该超曲面上的曲线沿绝热方向的曲率成比例,并且$g_{NL}$与该曲线的每单位弧长的曲率半径的变化有关。$f_{NL}$和$g_{NL}$可分别为阳性或阴性,但$τ_{NL}$必须为阳性且不小于$({6\over 5}f_{NL})^2$。

英文摘要:

In this paper we mainly focus on the curvature perturbation generated at the end of multi-field inflation, such as the multi-brid inflation. Since the curvature perturbation is produced on the super-horizon scale, the bispectrum and trispectrum have a local shape. The size of bispectrum is measured by $f_{NL}$ and the trispectrum is characterized by two parameters $τ_{NL}$ and $g_{NL}$. For simplicity, the trajectory of inflaton is assumed to be a straight line in the field space and then the entropic perturbations do not contribute to the curvature perturbation during inflation. As long as the background inflaton path is not orthogonal to the hyper-surface for inflation to end, the entropic perturbation can make a contribution to the curvature perturbation at the end of inflation and a large local-type non-Gaussiantiy is expected. An interesting thing is that the non-Gaussianity parameters are completely determined by the geometric properties of the hyper-surface of the end of inflation. For example, $f_{NL}$ is proportional to the curvature of the curve on this hyper-surface along the adiabatic direction and $g_{NL}$ is related to the change of the curvature radius per unit arc-length of this curve. Both $f_{NL}$ and $g_{NL}$ can be positive or negative respectively, but $τ_{NL}$ must be positive and not less than $({6\over 5}f_{NL})^2$.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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