# Cosmology with Stacked Cluster Weak Lensing and Cluster-Galaxy   Cross-Correlations

**Authors:** Andr\'es N. Salcedo, Benjamin D. Wibking, David H. Weinberg, Hao-Yi, Wu, Douglas Ferrer, Daniel Eisenstein, Philip Pinto

arXiv: 1906.06499 · 2019-11-06

## TL;DR

This paper demonstrates that combining cluster weak lensing with galaxy clustering measurements can precisely constrain cosmological parameters like _8, effectively breaking degeneracies and enabling internal consistency tests.

## Contribution

It introduces a method to combine _8-sensitive observables to achieve percent-level constraints, accounting for nuisance parameters and survey properties.

## Key findings

- Forecasts 0.8-1.4% _8 constraints with combined measurements.
- Shows comparable constraining power from small and large scale regimes.
- Enables internal consistency tests of the _8 measurement.

## Abstract

Cluster weak lensing is a sensitive probe of cosmology, particularly the amplitude of matter clustering $\sigma_8$ and matter density parameter $\Omega_m$. The main nuisance parameter in a cluster weak lensing cosmological analysis is the scatter between the true halo mass and the relevant cluster observable, denoted $\sigma_{\ln Mc}$. We show that combining the cluster weak lensing observable $\Delta \Sigma$ with the projected cluster-galaxy cross-correlation function $w_{p,cg}$ and galaxy auto-correlation function $w_{p,gg}$ can break the degeneracy between $\sigma_8$ and $\sigma_{\ln Mc}$ to achieve tight, percent-level constraints on $\sigma_8$. Using a grid of cosmological N-body simulations, we compute derivatives of $\Delta \Sigma$, $w_{p,cg}$, and $w_{p,gg}$ with respect to $\sigma_8$, $\Omega_m$, $\sigma_{\ln Mc}$ and halo occupation distribution (HOD) parameters describing the galaxy population. We also compute covariance matrices motivated by the properties of the Dark Energy Suvery (DES) cluster and weak lensing survey and the BOSS CMASS galaxy redshift survey. For our fiducial scenario combining $\Delta \Sigma$, $w_{p,cg}$, and $w_{p,gg}$ measured over $0.3-30.0 \; h^{-1} \; \mathrm{Mpc}$, for clusters at $z=0.35-0.55$ above a mass threshold $M_c\approx 2\times 10^{14} \; h^{-1} \; \mathrm{M_{\odot}}$, we forecast a $1.4\%$ constraint on $\sigma_8$ while marginalizing over $\sigma_{\ln Mc}$ and all HOD parameters. Reducing the mass threshold to $1\times 10^{14} \; h^{-1} \; \mathrm{M_{\odot}}$ and adding a $z=0.15-0.35$ redshift bin sharpens this constraint to $0.8\%$. The small scale $(r_p < 3.0 \; h^{-1} \; \mathrm{Mpc})$ ``mass function'' and large scale $(r_p > 3.0 \; h^{-1} \; \mathrm{Mpc})$ ``halo-mass cross-correlation'' regimes of $\Delta \Sigma$ have comparable constraining power, allowing internal consistency tests from such an analysis.

## Full text

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## Figures

12 figures with captions in the complete paper: https://tomesphere.com/paper/1906.06499/full.md

## References

128 references — full list in the complete paper: https://tomesphere.com/paper/1906.06499/full.md

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Source: https://tomesphere.com/paper/1906.06499