论文标题

通过相关来限制结构的增长率

Constraining the growth rate of structure with phase correlations

论文作者

Byun, Joyce, Franco, Felipe Oliveira, Howlett, Cullan, Bonvin, Camille, Obreschkow, Danail

论文摘要

我们表明,红移空间中星系密度场的阶段之间的相关性提供了有关与功率谱系互补的大规模结构增长率的其他信息。特别是,我们考虑了线相关函数(LCF)的多物,该函数(LCF)将相关的阶段相关联,并使用Fisher的预测方法来表明LCF多物可以打破结构$ f $的增长速率$ f $的增长速率与危险弹性的测量之间的变化,并且在大型量量中均具有量子量的量子量。这导致$ f $和$σ_8$的衡量结果提高了220%,对于$ k _ {\ rm max} = 0.15 \,H \ Mathrm {mpc}^{ - 1} $,高达50%,$ 50% H \ Mathrm {MPC}^{ - 1} $在RedShift $ z = 0.25 $,仅对于即将到来的Garaxy Surveys(例如Desi和Euclid)的发电频谱测量。 $ f $和$ f $ $ k _ {\ rm max} = 0.15 \,h \ mathrm {mpc}^{ - 1} $的平均约束的平均改善是$ \ sim 90 $ 90 $ sim per sim per,sim per centii per center per, $ \ Overline {z} = 1.25 $,$ \ sim 40 $ h $α$ a $ a $ alline {z} = 1.3 $。对于$ k _ {\ rm max} = 0.30 \,h \ mathrm {mpc}^{ - 1} $,对于Desi BGS样本的平均改进为$ \ sim 40 $ 40 $,$ \ sim 20 $ 20 $ 20 $ n desi elg和Euclid h $α$ al $ al $ al $ al $ alaxies。

We show that correlations between the phases of the galaxy density field in redshift space provide additional information about the growth rate of large-scale structure that is complementary to the power spectrum multipoles. In particular, we consider the multipoles of the line correlation function (LCF), which correlates phases between three collinear points, and use the Fisher forecasting method to show that the LCF multipoles can break the degeneracy between the measurement of the growth rate of structure $f$ and the amplitude of perturbations $σ_8$ that is present in the power spectrum multipoles at large scales. This leads to an improvement in the measurement of $f$ and $σ_8$ by up to 220 per cent for $k_{\rm max} = 0.15 \, h\mathrm{Mpc}^{-1}$ and up to 50 per cent for $k_{\rm max} = 0.30 \, h\mathrm{Mpc}^{-1}$ at redshift $z=0.25$, with respect to power spectrum measurements alone for the upcoming generation of galaxy surveys like DESI and Euclid. The average improvements in the constraints on $f$ and $σ_8$ for $k_{\rm max} = 0.15 \, h\mathrm{Mpc}^{-1}$ are $\sim 90$ per cent for the DESI BGS sample with mean redshift $\overline{z}=0.25$, $\sim 40$ per cent for the DESI ELG sample with $\overline{z}=1.25$, and $\sim 40$ per cent for the Euclid H$α$ galaxies with $\overline{z}=1.3$. For $k_{\rm max} = 0.30 \, h\mathrm{Mpc}^{-1}$, the average improvements are $\sim 40$ per cent for the DESI BGS sample and $\sim 20$ per cent for both the DESI ELG and Euclid H$α$ galaxies.

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