论文标题

除了黑暗能源费舍尔的预测之外:DESI将如何限制LCDM和典型模型

Beyond dark energy Fisher forecasts: how DESI will constrain LCDM and quintessence models

论文作者

Goldstein, Samuel, Park, Minsu, Raveri, Marco, Jain, Bhuvnesh, Samushia, Lado

论文摘要

我们以当前的宇宙学观察为基础,以两种方式预测暗能量光谱仪器(DESI)的功率:1。标准$λ$ CDM模型中参数组合的约束功率的增益和2。深色能量模型的重建。对于以前的任务,我们使用最近开发的形式主义来提取受宇宙学数据不同组合约束的主要参数组合。对于后者,我们使用有效的黑能场理论进行了非参数重建。使用对哈勃参数的模拟DESI观察,角直径距离和增长率,我们发现DESI将对$λ$ CDM和典型限制的当前数据集提供显着改进。包括DESI模拟在我们的$λ$ CDM分析中,改善了$ω_m$,$ H_0 $和$σ_8$的限制,其中几乎完全来自角色直径距离和结构测量的增长。我们的精髓重建表明,DESI将大大改善对一系列典型属性的约束,例如重建的电位,标量场旅行和状态的暗能量方程。在存在非$λ$ CDM信号的情况下,角直径距离测量值特别约束,其中无法通过$ h_0 $和$ω_m$的偏移来解释电位。

We baseline with current cosmological observations to forecast the power of the Dark Energy Spectroscopic Instrument (DESI) in two ways: 1. the gain in constraining power of parameter combinations in the standard $Λ$CDM model, and 2. the reconstruction of quintessence models of dark energy. For the former task we use a recently developed formalism to extract the leading parameter combinations constrained by different combinations of cosmological survey data. For the latter, we perform a non-parametric reconstruction of quintessence using the Effective Field Theory of Dark Energy. Using mock DESI observations of the Hubble parameter, angular diameter distance, and growth rate, we find that DESI will provide significant improvements over current datasets on $Λ$CDM and quintessence constraints. Including DESI mocks in our $Λ$CDM analysis improves constraints on $Ω_m$, $H_0$, and $σ_8$ by a factor of two, where the improvement results almost entirely from the angular diameter distance and growth of structure measurements. Our quintessence reconstruction suggests that DESI will considerably improve constraints on a range of quintessence properties, such as the reconstructed potential, scalar field excursion, and the dark energy equation of state. The angular diameter distance measurements are particularly constraining in the presence of a non-$Λ$CDM signal in which the potential cannot be accounted for by shifts in $H_0$ and $Ω_m$.

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