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arXiv 0909.0529astro-ph.CO
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弱透镜巡天中非高斯性的最佳捕获:功率谱、双谱和晕计数

Optimal capture of non-Gaussianity in weak lensing surveys: power spectrum, bispectrum and halo counts

Joel Berge, Adam Amara, Alexandre Refregier

摘要:

我们比较了弱透镜选择星系团计数和弱透镜双谱在捕获非高斯特征的暗物质分布的效率。我们使用晕模型来计算弱透镜功率谱,双谱和预期数量的检测到的集群,并推导出一个大的,低系统的弱透镜调查的宇宙学参数的约束,通过专注于$Ω_m$-$σ_8$平面和暗能量状态方程。我们将功率谱分成数据的已解决部分和未解决部分,已解决部分被定义为检测到的簇,未解决部分被定义为场的其余部分。我们考虑四种类型的集群计数,考虑到不同的信息量:信噪比峰值计数;作为集群质量的函数的计数;作为集群红移的函数的计数;以及作为集群质量和红移的函数的计数。我们表明,当结合功率谱,这四种计数提供了类似的约束,从而允许一个执行最直接的计数,信噪比峰值计数,并得到百分比水平的宇宙学参数的约束。我们表明,弱透镜双谱给出的约束条件与功率谱给出的约束条件相当,并捕获非高斯特征以及簇计数,其与功率谱的组合给出的宇宙学参数的误差类似于,如果不是稍微小于,当功率谱与簇计数相结合时获得的误差。最后,我们注意到,为了达到其潜力,弱透镜双谱必须使用所有三角形配置计算,因为等边三角形单独不提供有用的信息。

英文摘要:

We compare the efficiency of weak lensing-selected galaxy clusters counts and of the weak lensing bispectrum at capturing non-Gaussian features in the dark matter distribution. We use the halo model to compute the weak lensing power spectrum, the bispectrum and the expected number of detected clusters, and derive constraints on cosmological parameters for a large, low systematic weak lensing survey, by focusing on the $Ω_m$-$σ_8$ plane and on the dark energy equation of state. We separate the power spectrum into the resolved and the unresolved parts of the data, the resolved part being defined as detected clusters, and the unresolved part as the rest of the field. We consider four kinds of clusters counts, taking into account different amount of information : signal-to-noise ratio peak counts; counts as a function of clusters' mass; counts as a function of clusters' redshift; and counts as a function of clusters' mass and redshift. We show that when combined with the power spectrum, those four kinds of counts provide similar constraints, thus allowing one to perform the most direct counts, signal-to-noise peaks counts, and get percent level constraints on cosmological parameters. We show that the weak lensing bispectrum gives constraints comparable to those given by the power spectrum and captures non-Gaussian features as well as clusters counts, its combination with the power spectrum giving errors on cosmological parameters that are similar to, if not marginally smaller than, those obtained when combining the power spectrum with cluster counts. We finally note that in order to reach its potential, the weak lensing bispectrum must be computed using all triangle configurations, as equilateral triangles alone do not provide useful information.

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