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arXiv 0907.0486astro-ph.CO
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用弱透镜峰计数探测宇宙学

Probing Cosmology with Weak Lensing Peak Counts

Jan M. Kratochvil, Zoltán Haiman, Morgan May

摘要:

我们建议在弱透镜(WL)地图计数峰,作为其高度的函数,探测模型的暗能量和约束宇宙学参数。因为峰值可以直接在二维WL图中识别,所以它们可以提供约束,而不受识别和确定星系团质量时所涉及的潜在选择效应和偏差的影响。我们已经运行了宇宙学N体模拟,在三个模型中产生WL收敛图,这些模型具有不同的暗能量状态方程参数w=-0.8,-1和-1.2,具有固定的原始功率谱归一化(分别对应于当前的标准化σ 8 =0.742,0.798和0.839)。通过比较在-0.1 < kappa < 0.2的范围内的8个收敛箱中的WL峰值的数量,在单个模拟的3x 3度场的多个实现中,我们表明第一(最后)对模型可以在95%(85%)的置信水平下区分。深度和面积(20,000平方米)的调查度),与LSST的预期值相当,应具有大约的系数。50更好的参数灵敏度。我们发现,相对较低的振幅峰值(kappa = 0.03),这通常不对应于一个单一的崩溃晕沿视线,占这种敏感性的大部分。我们研究了一系列的平滑尺度和源星系的红移。在源星系密度固定为15/弧分^[2]的情况下,我们能够可靠地模拟的最小尺度(1弧分)可以提供最好的结果,z_s=2比z_s< 1.5的灵敏度要高得多。

英文摘要:

We propose counting peaks in weak lensing (WL) maps, as a function of their height, to probe models of dark energy and to constrain cosmological parameters. Because peaks can be identified in two-dimensional WL maps directly, they can provide constraints that are free from potential selection effects and biases involved in identifying and determining the masses of galaxy clusters. We have run cosmological N-body simulations to produce WL convergence maps in three models with different constant values of the dark energy equation of state parameter, w=-0.8, -1, and -1.2, with a fixed normalization of the primordial power spectrum (corresponding to present-day normalizations of sigma8=0.742, 0.798, and 0.839, respectively). By comparing the number of WL peaks in 8 convergence bins in the range of -0.1 < kappa < 0.2, in multiple realizations of a single simulated 3x3 degree field, we show that the first (last) pair of models can be distinguished at the 95% (85%) confidence level. A survey with depth and area (20,000 sq. degrees), comparable to those expected from LSST, should have a factor of approx. 50 better parameter sensitivity. We find that relatively low-amplitude peaks (kappa = 0.03), which typically do not correspond to a single collapsed halo along the line of sight, account for most of this sensitivity. We study a range of smoothing scales and source galaxy redshifts (z_s). With a fixed source galaxy density of 15/arcmin^2, the best results are provided by the smallest scale we can reliably simulate, 1 arcminute, and z_s=2 provides substantially better sensitivity than z_s< 1.5.

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