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arXiv 1504.01262astro-ph.CO
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聚集的暗能量如何影响物质扰动

How clustering dark energy affects matter perturbations

A. Mehrabi, S. Basilakos, F. Pace

摘要:

宇宙结构形成的速率在均匀和聚集的暗能量模型中是不同的。暗能量聚集的程度取决于其有效声速$c^{2}_{\rm eff}$的大小,对于$c_{\rm eff}=0$暗能量簇,其方式与暗物质相似,而对于$c_{\rm eff}=1$,其保持(近似)均匀。本文考虑了暗能量分量的两个不同的状态方程$w_{\rm d}=const$和$w_{\rm d}=w_0+w_1\left(\frac{z}{1+z}\right)$,并以$c_{\rm eff}$为自由参数,利用现有的SnIa、重子声振荡、CMB位移参数等数据,尝试约束暗能量的有效声速({ \em Planck}和{ \em WMAP}),哈勃参数,大爆炸核合成和结构$fσ_{8}(z)$的生长速率。首先,我们在假设$c_{\rm eff}=const$的条件下导出了支配暗物质和暗能量成团的方程的最一般形式。最后,进行总体似然分析,我们发现,似然函数的峰值在$c_{\rm eff}=0$,但暗能量声速是退化的宇宙学参数,即$Ω_{\rm m}$和$w_{\rm d}$。

英文摘要:

The rate of structure formation in the Universe is different in homogeneous and clustered dark energy models. The degree of dark energy clustering depends on the magnitude of its effective sound speed $c^{2}_{\rm eff}$ and for $c_{\rm eff}=0$ dark energy clusters in a similar fashion to dark matter while for $c_{\rm eff}=1$ it stays (approximately) homogeneous. In this paper we consider two distinct equations of state for the dark energy component, $w_{\rm d}=const$ and $w_{\rm d}=w_0+w_1\left(\frac{z}{1+z}\right)$ with $c_{\rm eff}$ as a free parameter and we try to constrain the dark energy effective sound speed using current available data including SnIa, Baryon Acoustic Oscillation, CMB shift parameter ({\em Planck} and {\em WMAP}), Hubble parameter, Big Bang Nucleosynthesis and the growth rate of structures $fσ_{8}(z)$. At first we derive the most general form of the equations governing dark matter and dark energy clustering under the assumption that $c_{\rm eff}=const$. Finally, performing an overall likelihood analysis we find that the likelihood function peaks at $c_{\rm eff}=0$, however the dark energy sound speed is degenerate with respect to the cosmological parameters, namely $Ω_{\rm m}$ and $w_{\rm d}$.

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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