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arXiv 2007.08998astro-ph.CO
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完成的SDSS-IV扩展重子振荡光谱巡天:红移0.8 - 2.2组态空间类星体样品各向异性成簇分析的BAO和RSD测量

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

Jiamin Hou, Ariel G. Sánchez, Ashley J. Ross, Alex Smith, Richard Neveux, Julian Bautista, Etienne Burtin, Cheng Zhao, Román Scoccimarro, Kyle S. Dawson, Arnaud… 展开作者

Jiamin Hou, Ariel G. Sánchez, Ashley J. Ross, Alex Smith, Richard Neveux, Julian Bautista, Etienne Burtin, Cheng Zhao, Román Scoccimarro, Kyle S. Dawson, Arnaud de Mattia, Axel de la Macorra, Hélion du Mas des Bourboux, Daniel J. Eisenstein, Héctor Gil-Marín, Brad W. Lyke, Faizan G. Mohammad, Eva-Maria Mueller, Will J. Percival, Mariana Vargas Magaña, Graziano Rossi, Pauline Zarrouk, Gong-Bo Zhao, Jonathan Brinkmann, Joel R. Brownstein, Chia-Hsun Chuang, Adam D. Myers, Jeffrey A. Newman, Donald P. Schneider, M. Vivek

摘要:

我们测量了斯隆数字巡天IV扩展重子振荡光谱巡天(eBOSS)数据发布16(DR 16)的类星体样本的各向异性聚类。一个$343,708$光谱确认的红移$0.8<z<2.2$之间的类星体样本被用作底层暗物质场的示踪剂。与DR 14样品相比,最终样品的对象数量和调查面积增加了一倍。本文通过测量两点相关函数,并利用勒让德多项式进行分解,给出了位形空间的分析。对于勒让德多极矩的全形分析,我们测量了BAO距离和宇宙结构的增长率。在$z_{\rm eff}=1.48$的有效红移处,我们测量了共动角直径距离$D_{\rm M}(z_{\rm eff})/r_{\rm drag} = 30.66\pm0.88$,哈勃距离$D_{\rm H}(z_{\rm eff})/r_{\rm drag} = 13.11\pm0.52$和生长率$fσ_8(z_{\rm eff}) = 0.439\pm0.048$。这些测量的准确性确认使用一套广泛的模拟模拟开发的类星体样本。相对于DR 14结果,距离和生长速率测量的不确定性已大幅降低($\sim 45\%$和PDMATHAMT)。我们还进行了仅BAO分析,以交叉检查全形状分析方法的稳健性。将我们的分析与傅立叶空间分析相结合,我们得到$D^{\bf{c}}_{\rm M}(z_{\rm eff})/r_{\rm drag} = 30.22 \pm 0.79$、$D^{\bf{c}}_{\rm H}(z_{\rm eff})/r_{\rm drag} = 13.26 \pm 0.47$和$fσ_8^{\bf{c}}(z_{\rm eff}) = 0.464 \pm 0.045$。

英文摘要:

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 $fσ_8^{\bf{c}}(z_{\rm eff}) = 0.464 \pm 0.045$.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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