论文标题
在$ z> 5 $的情况下探测与高分辨率的ly $α$森林光谱的热介质的热状态
Probing the thermal state of the intergalactic medium at $z>5$ with the transmission spikes in high-resolution Ly$α$ forest spectra
论文作者
论文摘要
我们比较了五个高分辨率,高$ $α$ forest光谱的样本,$ 6 <z \ lyssim 6.5 $ QSO,旨在旨在将剩余的剩余变速器钉在$ z> 5 $上,以及从Sherwood和Sherwood-Relics-Relysigic nivigig in nimbalsimaction of Sherwood-Relics套件中的模拟吸收光谱中获得的模拟吸收光谱所获得的(均来自$ z> 5 $)的含量。我们使用一个配置文件拟合程序来用于倒的传输通量,$ 1-F $,类似于下部红移的传输通量$ f $的广泛使用的VOIGT配置文件,以表征IGM的主要密集区域不足区域的变速器尖峰。我们能够使用均匀的紫外线背景和晚期抗离子模型的完全辐射传递模拟对变速器尖峰的宽度和高度分布进行光学薄模拟。我们发现,模拟透射尖峰的拟合成分的宽度非常敏感到电离IgM的瞬时温度。在IgM的低趋势模型中,尖峰的内部结构更为突出。 The width distribution of the observed transmission spikes, which require high spectral resolution ($\leq $ 8 km/s) to be resolved, is reproduced for optically thin simulations with a temperature at mean density of $T_0= (11000 \pm 1600,10500\pm 2100,12000 \pm 2200)$ K at $z= (5.4,5.6,5.8)$.这很弱取决于温度密度关系的斜率,该斜率比等温度更陡峭。在不均匀的,晚期的电源,全辐射转移模拟中,中性氢的岛屿持续到$ z \ sim5.3 $,观察到的传输尖峰的宽度分布与温度密度关系中空间波动引起的$ t_0 $的范围一致。
We compare a sample of five high-resolution, high S/N Ly$α$ forest spectra of bright $6<z \lesssim 6.5$ QSOs aimed at spectrally resolving the last remaining transmission spikes at $z>5$ with those obtained from mock absorption spectra from the Sherwood and Sherwood-Relics suites of hydrodynamical simulations of the intergalactic medium (IGM). We use a profile fitting procedure for the inverted transmitted flux, $1-F$, similar to the widely used Voigt profile fitting of the transmitted flux $F$ at lower redshifts, to characterise the transmission spikes that probe predominately underdense regions of the IGM. We are able to reproduce the width and height distributions of the transmission spikes, both with optically thin simulations of the post-reionization Universe using a homogeneous UV background and full radiative transfer simulations of a late reionization model. We find that the width of the fitted components of the simulated transmission spikes is very sensitive to the instantaneous temperature of the reionized IGM. The internal structures of the spikes are more prominant in low temeperature models of the IGM. The width distribution of the observed transmission spikes, which require high spectral resolution ($\leq $ 8 km/s) to be resolved, is reproduced for optically thin simulations with a temperature at mean density of $T_0= (11000 \pm 1600,10500\pm 2100,12000 \pm 2200)$ K at $z= (5.4,5.6,5.8)$. This is weakly dependent on the slope of the temperature-density relation, which is favoured to be moderately steeper than isothermal. In the inhomogeneous, late reionization, full radiative transfer simulations where islands of neutral hydrogen persist to $z\sim5.3$, the width distribution of the observed transmission spikes is consistent with the range of $T_0$ caused by spatial fluctuations in the temperature-density relation.