论文标题
完成的SDSS-IV扩展BARYON振荡光谱调查:来自各向异性聚类分析的BAO和RSD测量,对Redshift 0.8和2.2之间的构型样品进行了类星体样品的分析。
The Completed SDSS-IV extended Baryon Oscillation Spectroscopic Survey: BAO and RSD measurements from anisotropic clustering analysis of the Quasar Sample in configuration space between redshift 0.8 and 2.2
论文作者
论文摘要
我们从Sloan数字天空调查IV扩展Baryon振荡光谱调查(EBOSS)的数据版本16(DR16)中测量了类星体样品的各向异性聚类。在红移$ 0.8 <z <2.2 $之间,$ 343,708 $的样本用作基础暗物质领域的示踪剂。与DR14样品相比,最终样本将对象的数量和调查区域加倍。在本文中,我们通过测量两点相关函数并使用Legendre多项式分解来介绍配置空间中的分析。为了对Legendre Multile Moments的全形分析,我们测量了BAO距离和宇宙结构的生长速度。在有效的红移$ z {\ rm eff} = 1.48 $的情况下,我们测量了com的角直径距离$ d _ {\ rm m} {\ rm m}(z _ {\ rm eff})/r _ {\ rm _ {\ rm drag} h}(z _ {\ rm eff})/r _ {\ rm drag} = 13.11 \ pm0.52 $和增长率$fσ_8(z _ {\ rm eff})= 0.439 \ pm0.048 $。这些测量值的准确性是使用为类星体样本开发的大量模拟模拟确认的。相对于DR14结果,对距离和增长率测量值的不确定性已大大降低($ \ sim 45 \%$和$ \ sim30 \%$)。我们还执行仅BAO分析以跨越完整形状分析方法的鲁棒性。将我们的分析与傅立叶空间分析相结合,我们到达$ d^{\ bf {c}} _ {\ rm m} _ {\ rm m}(z _ {\ rm eff})/r _ {\ rm drag} = 30.22 \ 30.22 \ pm pm 0.79 $,$ d^$,$ d^{\ bf { eff})/r _ {\ rm drag} = 13.26 \ pm 0.47 $,$fσ_8^{\ bf {c}}}}}}(z _ {\ rm eff})= 0.464 \ pm 0.045 $。
We measure the anisotropic clustering of the quasar sample from Data Release 16 (DR16) of the Sloan Digital Sky Survey IV extended Baryon Oscillation Spectroscopic Survey (eBOSS). A sample of $343,708$ spectroscopically confirmed quasars between redshift $0.8<z<2.2$ are used as tracers of the underlying dark matter field. In comparison with DR14 sample, the final sample doubles the number of objects as well as the survey area. In this paper, we present the analysis in configuration space by measuring the two-point correlation function and decompose using the Legendre polynomials. For the full-shape analysis of the Legendre multipole moments, we measure the BAO distance and the growth rate of the cosmic structure. At an effective redshift of $z_{\rm eff}=1.48$, we measure the comoving angular diameter distance $D_{\rm M}(z_{\rm eff})/r_{\rm drag} = 30.66\pm0.88$, the Hubble distance $D_{\rm H}(z_{\rm eff})/r_{\rm drag} = 13.11\pm0.52$, and the growth rate $fσ_8(z_{\rm eff}) = 0.439\pm0.048$. The accuracy of these measurements is confirmed using an extensive set of mock simulations developed for the quasar sample. The uncertainties on the distance and growth rate measurements have been reduced substantially ($\sim 45\%$ and $\sim30\%$) with respect to the DR14 results. We also perform a BAO-only analysis to cross check the robustness of the methodology of the full-shape analysis. Combining our analysis with the Fourier space analysis, we arrive at $D^{\bf{c}}_{\rm M}(z_{\rm eff})/r_{\rm drag} = 30.22 \pm 0.79$, $D^{\bf{c}}_{\rm H}(z_{\rm eff})/r_{\rm drag} = 13.26 \pm 0.47$, and $fσ_8^{\bf{c}}(z_{\rm eff}) = 0.464 \pm 0.045$.