论文标题

Kids-1000宇宙学:限制额外的$λ$ CDM

KiDS-1000 Cosmology: constraints beyond flat $Λ$CDM

论文作者

Tröster, Tilman, Asgari, Marika, Blake, Chris, Cataneo, Matteo, Heymans, Catherine, Hildebrandt, Hendrik, Joachimi, Benjamin, Lin, Chieh-An, Sánchez, Ariel G., Wright, Angus H., Bilicki, Maciej, Bose, Benjamin, Crocce, Martin, Dvornik, Andrej, Erben, Thomas, Giblin, Benjamin, Glazebrook, Karl, Hoekstra, Henk, Joudaki, Shahab, Kannawadi, Arun, Köhlinger, Fabian, Kuijken, Konrad, Lidman, Chris, Lombriser, Lucas, Mead, Alexander, Parkinson, David, Shan, HuanYuan, Wolf, Christian, Xia, Qianli

论文摘要

我们通过改变空间曲率$ω_k$,中微子群众$ \ summ_ν$,状态参数$ w $ $ w $的暗能量方程和hu-sawicki $ f(r)$ f(r)$ f(r)$ f(r)$ f _ r0} $ f_ r0} $ f_ r0} $ f_ r0} $ f _ r0}。 With the combined $3\times2$pt measurements of cosmic shear from the Kilo-Degree Survey (KiDS-1000), galaxy clustering from the Baryon Oscillation Spectroscopic Survey (BOSS), and galaxy-galaxy lensing from the overlap between KiDS-1000, BOSS, and the spectroscopic 2-degree Field Lensing Survey (2dFLenS), we find results that are fully consistent with a flat $λ$ CDM型号,带有$ω__k= 0.011^{+0.054} _ { - 0.057} $,$ \ summ_ν<1.76 $ ev(95%Cl)和$ W = -0.99^{+0.11} _ {+0.11} _ { - 0.13} $。 $ f_ {r0} $参数在我们的完全非线性$ f(r)$ cosmic剪切分析中不受限制。考虑到三个不同的模型选择标准,我们发现对基准扁平$λ$ CDM模型或任何考虑的扩展名都没有明确的偏好。除了扩展到平坦的$λ$ CDM参数空间外,我们还通过将原始功率谱的振幅固定到Planck最佳拟合值,并从CMB的超级Novae和镜头中添加外部数据,还通过将原始功率谱的幅度固定为Flat $λ$ CDM参数空间的常见子集的限制。此分析中的超出$λ$ CDM型号和所探索的限制都无法在$ 3 \ times2 $ pt约束和普朗克之间解决$ \ sim3σ$张力,除$ w $ cdm外,在$ w $ cdm的情况下,$ s_8 $ s_8 $张力均已恢复。但是,在考虑关节$ S_8 $ - $ W $参数空间时,$ W $ CDM CASE中的张力仍然存在。发现联合扁平$λ$ CDM CMB镜头和$ 3 \ times2 $ pt分析可在$ω_ {\ rm m} = 0.307^{+0.008} _ { - 0.013} $,$σ_8= 0.769 = 0.769^{+0.769^{+0.769^{$ 0.769^{$ 0.769^{$ 0.769^{$ 0.022} _ {$ 0.769 = 0.022} _ {$ 0.022} _} _ {+0.013} _ { - 0.013} _ {+0.013} _ { - 0.022} _} $ s_8 = 0.779^{+0.013} _ { - 0.013} $。

We present constraints on extensions to the flat $Λ$CDM cosmological model by varying the spatial curvature $Ω_K$, the sum of the neutrino masses $\sum m_ν$, the dark energy equation of state parameter $w$, and the Hu-Sawicki $f(R)$ gravity $f_{R0}$ parameter. With the combined $3\times2$pt measurements of cosmic shear from the Kilo-Degree Survey (KiDS-1000), galaxy clustering from the Baryon Oscillation Spectroscopic Survey (BOSS), and galaxy-galaxy lensing from the overlap between KiDS-1000, BOSS, and the spectroscopic 2-degree Field Lensing Survey (2dFLenS), we find results that are fully consistent with a flat $Λ$CDM model with $Ω_K=0.011^{+0.054}_{-0.057}$, $\sum m_ν<1.76$ eV (95% CL), and $w=-0.99^{+0.11}_{-0.13}$. The $f_{R0}$ parameter is unconstrained in our fully non-linear $f(R)$ cosmic shear analysis. Considering three different model selection criteria, we find no clear preference for either the fiducial flat $Λ$CDM model or any of the considered extensions. Besides extensions to the flat $Λ$CDM parameter space, we also explore restrictions to common subsets of the flat $Λ$CDM parameter space by fixing the amplitude of the primordial power spectrum to the Planck best-fit value, as well as adding external data from supernovae and lensing of the CMB. Neither the beyond-$Λ$CDM models nor the imposed restrictions explored in this analysis are able to resolve the $\sim 3σ$ tension in $S_8$ between the $3\times2$pt constraints and Planck, with the exception of $w$CDM, where the $S_8$ tension is resolved. The tension in the $w$CDM case persists, however, when considering the joint $S_8$-$w$ parameter space. The joint flat $Λ$CDM CMB lensing and $3\times2$pt analysis is found to yield tight constraints on $Ω_{\rm m}=0.307^{+0.008}_{-0.013}$, $σ_8=0.769^{+0.022}_{-0.010}$, and $S_8=0.779^{+0.013}_{-0.013}$.

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