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首页> 外文期刊>PASJ: Publications of the Astronomical Society of Japan >SILVERRUSH. VI. A simulation of Lyα emitters in the reionization epoch and a comparison with Subaru Hyper Suprime-Cam survey early data
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SILVERRUSH. VI. A simulation of Lyα emitters in the reionization epoch and a comparison with Subaru Hyper Suprime-Cam survey early data

机译:银。 VI。电离时代Lyα发射体的模拟以及与Subaru Hyper Suprime-Cam调查早期数据的比较

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The survey of Lyman α emitters (LAEs) with the Subaru Hyper Suprime-Cam, called SILVERRUSH (Ouchi et?al. 2018, PASJ, 70, S13), is producing massive data of LAEs at z ? 6. Here we present LAE simulations to compare the SILVERRUSH data. In 1623 comoving Mpc3 boxes, where numerical radiative transfer calculations of reionization were performed, LAEs have been modeled with physically motivated analytic recipes as a function of halo mass. We have examined 23 models depending on the presence or absence of dispersion of halo Lyα emissivity, dispersion of the halo Lyα optical depth, τα, and halo mass dependence of τα. The unique free parameter in our model, a pivot value of τα, is calibrated so as to reproduce the z?=?5.7 Lyα luminosity function (LF) of SILVERRUSH. We compare our model predictions with Lyα LFs at z?=?6.6 and 7.3, LAE angular auto-correlation functions (ACFs) at z?=?5.7 and 6.6, and LAE fractions in Lyman break galaxies at 5??z??7. The Lyα LFs and ACFs are reproduced by multiple models, but the LAE fraction turns out to be the most critical test. The dispersion of τα and the halo mass dependence of τα are essential to explain all observations reasonably. Therefore, a simple model of one-to-one correspondence between halo mass and Lyα luminosity with a constant Lyα escape fraction has been ruled out. Based on our best model, we present a formula to estimate the intergalactic neutral hydrogen fraction, |$x_{m H, small {I}}$|?, from the observed Lyα luminosity density at z ? 6. We finally obtain |$x_{m H, small {I}}=0.5_{-0.3}^{+0.1}$| as a volume-average at z?=?7.3.
机译:用称为SILVERRUSH的Subaru Hyper Suprime-Cam对Lymanα发射器(LAE)进行的调查(Ouchi et al.2018,PASJ,70,S13)正在产生z处的大量LAEs数据。 6.在这里,我们介绍LAE仿真以比较SILVERRUSH数据。在1623个移动的Mpc3盒中,在其中进行了离子化的数值辐射转移计算,LAE的建模是基于物理动机的分析配方作为光晕质量的函数。我们已经检查了23个模型,具体取决于是否存在光晕Lyα发射率的色散,光晕Lyα光学深度的色散,τα和光晕质量对τα的依赖性。校准了我们模型中唯一的自由参数,即枢轴值τα,以便重现SILVERRUSH的zα=?5.7Lyα光度函数(LF)。我们将模型预测与z?=?6.6和7.3的LyαLFs,z?=?5.7和6.6的LAE角自相关函数(ACFs)以及5?<?z?< 7。 LyαLF和ACF可通过多种模型复制,但LAE分数却是最关键的测试。 τα的离散度和τα的晕圈质量依赖性对于合理地解释所有观察结果至关重要。因此,已经排除了晕圈质量和Lyα发光度与恒定的Lyα逃逸分数之间一一对应的简单模型。基于我们的最佳模型,我们提供了一个公式,用于根据在z?处观察到的Lyα光度密度来估算星系间中性氢分数| $ x _ { rm H , small {I}} $ |?。 6.我们最终获得| $ x _ { rm H , small {I}} = 0.5 _ {-0.3} ^ {+ 0.1} $ |在z≥7.3时作为体积平均值。

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