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arXiv 0904.0675hep-phastro-ph.COhep-th
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经典暴胀中的引力再加热

Gravitational reheating in quintessential inflation

E. J. Chun, S. Scopel, I. Zaballa

摘要:

我们提供了一个详细的研究引力再加热在典型的通货膨胀推广以前的分析只适用于标准的情况下,通货膨胀之后,由辐射的能量密度占主导地位的时代。典型的暴胀假设暴胀和宇宙的暗能量有一个共同的起源。在这种情况下,再加热可以通过暴胀-动能转换期间的引力粒子产生而发生。我们用数值计算了辐射能量密度的大小,并确定了辐射开始占主导地位的温度$T_*$。$T_*$的值由膨胀期间的哈勃参数$H_0$和过渡时间$Δt$控制,对于$H_0 Δt \ll1$,按比例缩放为$H_0^2 [\ln(1/H_0Δt)]^{3/4}$,对于$H_0Δt \gg 1$,按比例缩放为$H_0^2 (H_0 Δt)^{-c}$。模型相关的参数$c$被发现是在两个不同的参数化通货膨胀和kination之间的过渡约为0.5。

英文摘要:

We provide a detailed study of gravitational reheating in quintessential inflation generalizing previous analyses only available for the standard case when inflation is followed by an era dominated by the energy density of radiation. Quintessential inflation assumes a common origin for inflation and the dark energy of the Universe. In this scenario reheating can occur through gravitational particle production during the inflation-kination transition. We calculate numerically the amount of the radiation energy density, and determine the temperature $T_*$ at which radiation starts dominating over kination. The value of $T_*$ is controlled by the Hubble parameter $H_0$ during inflation and the transition time $Δt$, scaling as $H_0^2 [\ln(1/H_0Δt)]^{3/4}$ for $H_0 Δt \ll1$ and $H_0^2 (H_0 Δt)^{-c}$ for $H_0Δt \gg 1$. The model-dependent parameter $c$ is found to be around 0.5 in two different parametrizations for the transition between inflation and kination.

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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