4.7 Article

Weak-lensing statistics from the Coyote Universe

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 418, Issue 1, Pages 536-544

Publisher

OXFORD UNIV PRESS
DOI: 10.1111/j.1365-2966.2011.19502.x

Keywords

cosmology: theory; large-scale structure of Universe

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Analysing future weak-lensing data sets from KIDS, Dark Energy Survey (DES), LSST, Euclid and WFIRST requires precise predictions for the weak-lensing measures. In this paper, we present a weak-lensing prediction code based on the Coyote Universe emulator. The Coyote Universe emulator predicts the (non-linear) power spectrum of density fluctuations (P-delta) to high accuracy for k is an element of [0.002; 3.4] h Mpc(-1) within the redshift interval z is an element of [0; 1]; outside this regime, we extend P-delta using a modified HALOFIT code. This pipeline is used to calculate various second-order cosmic shear statistics, e. g., shear power spectrum, shear-shear correlation function, ring statistics and Complete Orthogonal Set of EB-mode Integrals (COSEBIs), and we examine how the upper limit in k (and z), to which P-delta is known, impacts on these statistics. For example, we find that k(max) similar to 8 h Mpc(-1) causes a bias in the shear power spectrum at l similar to 4000 that is comparable to the statistical errors (intrinsic shape noise and cosmic variance) of a DES-like survey, whereas for LSST-like errors k(max) similar to 15 h Mpc(-1) is needed to limit the bias at l similar to 4000. For the most recently developed second-order shear statistics, the COSEBIs, we find that nine modes can be calculated accurately knowing P-delta to k(max) = 10 h Mpc(-1). The COSEBIs allow for an EB-mode decomposition using a shear-shear correlation function measured over a finite range, thereby avoiding any EB-mode mixing due to finite survey size. We perform a detailed study in a five-dimensional parameter space in order to examine whether all cosmological information is captured by these nine modes with the result that already 7-8 modes are sufficient.

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