arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 1409.7205astro-ph.COgr-qchep-phhep-th
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用最近的观测包括红移空间畸变探索相互作用暗能量模型的全参数空间:参数化后弗里德曼方法的应用

Exploring the full parameter space for an interacting dark energy model with recent observations including redshift-space distortions: Application of the parametrized post-Friedmann approach

Yun-He Li, Jing-Fei Zhang, Xin Zhang

摘要:

暗能量可以改变暗物质的动力学,如果它们之间存在直接的相互作用。因此,测量结构生长,例如,红移空间畸变(RSD)是一个强有力的工具来约束相互作用暗能量(IDE)模型。对于广泛研究的$Q=3βHρ_{de}$模型,以前的工作表明,只有一个非常小的耦合($β\sim\mathcal{O}(10^{-3})$)可以生存在目前的RSD数据。然而,由于IDE情景中存在大规模不稳定性,所有这些分析都必须假设$w>-1$和$β>0$。在我们最近的工作[Phys. Rev. D 90,063005(2014)]中,我们通过为IDE场景建立参数化后弗里德曼(PPF)框架,成功解决了这个大规模不稳定性问题。因此,我们第一次有能力探索IDE模型的完整参数空间。在这项工作中,我们重新审视的观测约束的PPF框架内的$Q=3βHρ_{de}$模型。利用普朗克数据、重子声学振荡数据、超新星JLA样本和哈勃常数测量,得到了$β=-0.010^{+0.037}_{-0.033}$($1σ$)。在分析中进一步合并RSD数据后,拟合结果变为$β=-0.0148^{+0.0100}_{-0.0089}$($1σ$)。借助于RSD数据,$β$的误差大大减小。与以往的结果相比,我们的结果表明,一个负的$β$是有利的,目前的观测,并允许相对较大的相互作用率由目前的RSD数据。

英文摘要:

Dark energy can modify the dynamics of dark matter if there exists a direct interaction between them. Thus a measurement of the structure growth, e.g., redshift-space distortions (RSD), can provide a powerful tool to constrain the interacting dark energy (IDE) models. For the widely studied $Q=3βHρ_{de}$ model, previous works showed that only a very small coupling ($β\sim\mathcal{O}(10^{-3})$) can survive in current RSD data. However, all these analyses had to assume $w>-1$ and $β>0$ due to the existence of the large-scale instability in the IDE scenario. In our recent work [Phys. Rev. D 90, 063005 (2014)], we successfully solved this large-scale instability problem by establishing a parametrized post-Friedmann (PPF) framework for the IDE scenario. So we, for the first time, have the ability to explore the full parameter space of the IDE models. In this work, we reexamine the observational constraints on the $Q=3βHρ_{de}$ model within the PPF framework. By using the Planck data, the baryon acoustic oscillation data, the JLA sample of supernovae, and the Hubble constant measurement, we get $β=-0.010^{+0.037}_{-0.033}$ ($1σ$). The fit result becomes $β=-0.0148^{+0.0100}_{-0.0089}$ ($1σ$) once we further incorporate the RSD data in the analysis. The error of $β$ is substantially reduced with the help of the RSD data. Compared with the previous results, our results show that a negative $β$ is favored by current observations, and a relatively larger interaction rate is permitted by current RSD data.

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