The impact of correlated projections on weak lensing cluster counts

TL;DR

This study investigates how correlated large-scale structures affect weak lensing cluster counts, demonstrating that with proper filtering, their impact on mass estimates is minimal and the peak abundance scales predictably with cosmology.

Contribution

It shows that the impact of correlated projections on weak lensing peak counts can be minimized with optimal filtering and that the peak abundance scales with cosmology similarly to 3D mass functions.

Findings

Correlated projections contribute less than 2% to peak mass estimates with optimal filtering.

Peak abundance scales with cosmology in the same way as 3D mass functions.

Modified Sheth-Tormen fits describe peak counts within 10-20% accuracy.

Abstract

Large-scale structure projections are an obstacle in converting the shear signal of clusters detected in weak-lensing maps into virial masses. However, this step is not necessary for constraining cosmology with the shear-peak abundance, if we are able to predict its amplitude. We generate a large ensemble of N-body simulations spanning four cosmological models, with total volume V~1 (Gpc/h)^3 per model. Variations to the matter density parameter and amplitude of fluctuations are considered. We measure the abundance of peaks in the mass density projected in ~100 Mpc/h slabs to determine the impact of structures spatially correlated with the simulation clusters, identified by the 3D friends-of-friends algorithm. The halo model shows that the choice of the smoothing filter for the density field is important in reducing the contribution of correlated projections to individual halo masses. Such contributions are less than 2% in the case of the optimal, compensated filter used throughout this analysis. We measure the change in the mass of peaks when projected in slabs of various thicknesses. Peaks in slabs of 26 Mpc/h and 102 Mpc/h suffer an average mass change of less than 2% compared to their mass in slabs of 51 Mpc/h. We then explore the cosmology dependence of the projected-peak mass function, and find that, for a wide range of slab thicknesses (<500 Mpc/h), it scales with cosmology in exactly the same way as the 3D friends-of-friends mass function and the Sheth-Tormen formula. This extends the earlier result of Marian et al. (2009). Finally, we show that for all cosmological models considered, the low and intermediate mass bins of the peak abundance can be described using a modified Sheth-Tormen functional form to within 10%-20% accuracy.