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arXiv 0909.5210astro-ph.CO
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2.2 < z < 4.2 Lyman-alpha森林小尺度结构的度量

A Measurement of Small Scale Structure in the 2.2 < z < 4.2 Lyman-alpha Forest

Adam Lidz, C. -A. Faucher-Giguere, Aldo Dall'Aglio, Matthew McQuinn, Cora Fechner, Matias Zaldarriaga, Lars Hernquist, Suvendra Dutta

摘要:

Ly-a森林在小空间尺度上的波动幅度对IGM的温度及其空间波动敏感。IGM的温度及其空间变化包含了氢和氦再电离的重要信息。我们提出了一个新的测量的小尺度结构的Ly-a森林从40高分辨率,高信噪比,VLT光谱在z=2.2-4.2。我们卷积每个Ly-a森林光谱与适当选择的小波滤波器,这使我们能够提取森林中的小尺度结构的量作为每个光谱的位置的函数。我们将这些测量结果与跟踪超过20亿个粒子的Ly-a森林的高分辨率流体动力学模拟进行比较。这一比较表明,接近宇宙平均密度(T_0)的IGM温度在z=3.4附近达到峰值,在2-sigma置信度下,该点大于20,000 K。在z=3.4附近达到峰值温度后,较低红移处的温度与绝热冷却($T_0 \propto (1+z)^2$)预期的下降一致。在z=4.2时,我们的结果倾向于T_0 = 15- 20,000 K。然而,由于在此红移处平均透射通量的不确定性,一个T_0 = 10,000 K的冷IGM模型在2 σ水平上是不受欢迎的,尽管这样的冷IGM模型与z ~ 3-3.4的测量值有很大的差异。我们没有检测到大的空间波动的IGM温度在任何红移覆盖我们的数据集。对我们的测量结果最简单的解释是,HeII再电离在z ~ 3.4附近的某个时候完成,尽管统计不确定性仍然很大。

英文摘要:

The amplitude of fluctuations in the Ly-a forest on small spatial scales is sensitive to the temperature of the IGM and its spatial fluctuations. The temperature of the IGM and its spatial variations contain important information about hydrogen and helium reionization. We present a new measurement of the small-scale structure in the Ly-a forest from 40 high resolution, high signal-to-noise, VLT spectra at z=2.2-4.2. We convolve each Ly-a forest spectrum with a suitably chosen wavelet filter, which allows us to extract the amount of small-scale structure in the forest as a function of position across each spectrum. We compare these measurements with high resolution hydrodynamic simulations of the Ly-a forest which track more than 2 billion particles. This comparison suggests that the IGM temperature close to the cosmic mean density (T_0) peaks near z=3.4, at which point it is greater than 20,000 K at 2-sigma confidence. The temperature at lower redshift is consistent with the fall-off expected from adiabatic cooling ($T_0 \propto (1+z)^2$), after the peak temperature is reached near z=3.4. At z=4.2 our results favor a temperature of T_0 = 15-20,000 K. However, owing mostly to uncertainties in the mean transmitted flux at this redshift, a cooler IGM model with T_0 = 10,000 K is only disfavored at the 2-sigma level here, although such cool IGM models are strongly discrepant with the z ~ 3-3.4 measurement. We do not detect large spatial fluctuations in the IGM temperature at any redshift covered by our data set. The simplest interpretation of our measurements is that HeII reionization completes sometime near z ~ 3.4, although statistical uncertainties are still large [Abridged].

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