论文标题
通过加拿大氢强度映射实验检测宇宙学21 cm发射
Detection of Cosmological 21 cm Emission with the Canadian Hydrogen Intensity Mapping Experiment
论文作者
论文摘要
我们提出了通过加拿大氢强度映射实验(Chime)制成的红移0.78和1.43之间从大规模结构(LSS)发射的21厘米发射的。在102晚中获得的无线电观察用于构建图像,这些图被前景过滤并堆叠在发光红星系(LRG)(LRG),发射线星系(ELG)和Quasars(QSO)的角度和光谱位置上。我们发现在堆叠LSS的所有三个示踪剂上,贝叶斯因子的对数等于18.9(LRG),10.8(ELG)和56.3(QSO)时,我们发现了检测的决定性证据。基于似然比测试的另一种频繁解释,其检测意义为$7.1σ$(LRG),$5.7σ$(ELG)和$11.1σ$(QSO)。这些是使用干涉仪进行的第一个21厘米强度映射测量。我们约束中性氢(HI)的有效聚类幅度,定义为$ \ Mathcal {a} _ {\ rm hi} \ equiv 10^{3} \,ω__\ Mathrm {hi} $ω__\ MATHRM {HI} $是HI的宇宙丰度,$ B_ \ Mathrm {Hi} $是HI的线性偏置,$ \ langle \,Fμ^{2} \ rangle = 0.552 $编码在linear corder corder linear corders linear corders linear corders in linear corders in linear corder cord的影响。我们找到$ \ MATHCAL {a} _ \ MATHRM {HI} = 1.51^{+3.60} _ { - 0.97} $ for LRGS $(z = 0.84)$,$ \ MATHCAL {A} _ \ MATHRM {A} _ \ MATHRM {hi} = 6.76 = 6.76^$ 3.9.76^3.9.9.79 { $(z = 0.96)$,以及$ \ mathcal {a} _ \ mathrm {hi} = 1.68^{+1.10} _ { - 0.67} $ for qSOS $(z = 1.20)$,其约束因在非线性尺度上建模不确定性而受到限制。我们还对每个示踪剂的光谱红移敏感,并找到QSOS的非零偏置$δ\,v = -66 \ pm 20 \ mathrm {km/s} $。我们将QSO目录分为三个红移箱,每个红移箱都具有决定性的检测,$ z = 1.30 $ $ z = 1.30 $,迄今为止,最高的红移21厘米强度映射测量值。
We present a detection of 21-cm emission from large-scale structure (LSS) between redshift 0.78 and 1.43 made with the Canadian Hydrogen Intensity Mapping Experiment (CHIME). Radio observations acquired over 102 nights are used to construct maps which are foreground filtered and stacked on the angular and spectral locations of luminous red galaxies (LRG), emission line galaxies (ELG), and quasars (QSO) from the eBOSS clustering catalogs. We find decisive evidence for a detection when stacking on all three tracers of LSS, with the logarithm of the Bayes Factor equal to 18.9 (LRG), 10.8 (ELG), and 56.3 (QSO). An alternative frequentist interpretation, based on the likelihood-ratio test, yields a detection significance of $7.1σ$ (LRG), $5.7σ$ (ELG), and $11.1σ$ (QSO). These are the first 21-cm intensity mapping measurements made with an interferometer. We constrain the effective clustering amplitude of neutral hydrogen (HI), defined as $\mathcal{A}_{\rm HI}\equiv 10^{3}\,Ω_\mathrm{HI}\left(b_\mathrm{HI}+\langle\,fμ^{2}\rangle\right)$, where $Ω_\mathrm{HI}$ is the cosmic abundance of HI, $b_\mathrm{HI}$ is the linear bias of HI, and $\langle\,fμ^{2}\rangle=0.552$ encodes the effect of redshift-space distortions at linear order. We find $\mathcal{A}_\mathrm{HI}=1.51^{+3.60}_{-0.97}$ for LRGs $(z=0.84)$, $\mathcal{A}_\mathrm{HI}=6.76^{+9.04}_{-3.79}$ for ELGs $(z=0.96)$, and $\mathcal{A}_\mathrm{HI}=1.68^{+1.10}_{-0.67}$ for QSOs $(z=1.20)$, with constraints limited by modeling uncertainties at nonlinear scales. We are also sensitive to bias in the spectroscopic redshifts of each tracer, and find a non-zero bias $Δ\,v= -66 \pm 20 \mathrm{km/s}$ for the QSOs. We split the QSO catalog into three redshift bins and have a decisive detection in each, with the upper bin at $z=1.30$ producing the highest redshift 21-cm intensity mapping measurement thus far.