17 research outputs found

    Cosmological constraints from HSC survey first-year data using deep learning

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    We present cosmological constraints from the Subaru Hyper Suprime-Cam (HSC) first-year weak lensing shear catalogue using convolutional neural networks (CNNs) and conventional summary statistics. We crop 19 3×3 deg23\times3\,\mathrm{{deg}^2} sub-fields from the first-year area, divide the galaxies with redshift 0.3≤z≤1.50.3\le z\le1.5 into four equally-spaced redshift bins, and perform tomographic analyses. We develop a pipeline to generate simulated convergence maps from cosmological NN-body simulations, where we account for effects such as intrinsic alignments (IAs), baryons, photometric redshift errors, and point spread function errors, to match characteristics of the real catalogue. We train CNNs that can predict the underlying parameters from the simulated maps, and we use them to construct likelihood functions for Bayesian analyses. In the Λ\Lambda cold dark matter model with two free cosmological parameters Ωm\Omega_\mathrm{m} and σ8\sigma_8, we find Ωm=0.278−0.035+0.037\Omega_\mathrm{m}=0.278_{-0.035}^{+0.037}, S8≡(Ωm/0.3)0.5σ8=0.793−0.018+0.017S_8\equiv(\Omega_\mathrm{m}/0.3)^{0.5}\sigma_8=0.793_{-0.018}^{+0.017}, and the IA amplitude AIA=0.20−0.58+0.55A_\mathrm{IA}=0.20_{-0.58}^{+0.55}. In a model with four additional free baryonic parameters, we find Ωm=0.268−0.036+0.040\Omega_\mathrm{m}=0.268_{-0.036}^{+0.040}, S8=0.819−0.024+0.034S_8=0.819_{-0.024}^{+0.034}, and AIA=−0.16−0.58+0.59A_\mathrm{IA}=-0.16_{-0.58}^{+0.59}, with the baryonic parameters not being well-constrained. We also find that statistical uncertainties of the parameters by the CNNs are smaller than those from the power spectrum (5--24 percent smaller for S8S_8 and a factor of 2.5--3.0 smaller for Ωm\Omega_\mathrm{m}), showing the effectiveness of CNNs for uncovering additional cosmological information from the HSC data. With baryons, the S8S_8 discrepancy between HSC first-year data and Planck 2018 is reduced from ∼2.2 σ\sim2.2\,\sigma to 0.3–0.5 σ0.3\text{--}0.5\,\sigma.Comment: 22 pages, 14 figure

    Revealing the cosmic web dependent halo bias

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    Halo bias is the one of the key ingredients of the halo models. It was shown at a given redshift to be only dependent, to the first order, on the halo mass. In this study, four types of cosmic web environments: clusters, filaments, sheets and voids are defined within a state of the art high resolution NN-body simulation. Within those environments, we use both halo-dark matter cross-correlation and halo-halo auto correlation functions to probe the clustering properties of halos. The nature of the halo bias differs strongly among the four different cosmic web environments we describe. With respect to the overall population, halos in clusters have significantly lower biases in the {1011.0∼1013.5h−1M⊙10^{11.0}\sim 10^{13.5}h^{-1}\rm M_\odot} mass range. In other environments however, halos show extremely enhanced biases up to a factor 10 in voids for halos of mass {∼1012.0h−1M⊙\sim 10^{12.0}h^{-1}\rm M_\odot}. Such a strong cosmic web environment dependence in the halo bias may play an important role in future cosmological and galaxy formation studies. Within this cosmic web framework, the age dependency of halo bias is found to be only significant in clusters and filaments for relatively small halos \la 10^{12.5}\msunh.Comment: 14 pages, 14 figures, ApJ accepte

    Comparing weak lensing peak counts in baryonic correction models to hydrodynamical simulations

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    Next-generation weak lensing (WL) surveys, such as by the Vera Rubin Observatory's LSST, the Roman\textit{Roman} Space Telescope, and the Euclid\textit{Euclid} space mission, will supply vast amounts of data probing small, highly nonlinear scales. Extracting information from these scales requires higher-order statistics and the controlling of related systematics such as baryonic effects. To account for baryonic effects in cosmological analyses at reduced computational cost, semi-analytic baryonic correction models (BCMs) have been proposed. Here, we study the accuracy of BCMs for WL peak counts, a well studied, simple, and effective higher-order statistic. We compare WL peak counts generated from the full hydrodynamical simulation IllustrisTNG and a baryon-corrected version of the corresponding dark matter-only simulation IllustrisTNG-Dark. We apply galaxy shape noise expected at the depths reached by DES, KiDS, HSC, LSST, Roman\textit{Roman}, and Euclid\textit{Euclid}. We find that peak counts in BCMs are (i) accurate at the percent level for peaks with S/N<4\mathrm{S/N}<4, (ii) statistically indistinguishable from IllustrisTNG in most current and ongoing surveys, but (iii) insufficient for deep future surveys covering the largest solid angles, such as LSST and Euclid\textit{Euclid}. We find that BCMs match individual peaks accurately, but underpredict the amplitude of the highest peaks. We conclude that existing BCMs are a viable substitute for full hydrodynamical simulations in cosmological parameter estimation from beyond-Gaussian statistics for ongoing and future surveys with modest solid angles. For the largest surveys, BCMs need to be refined to provide a more accurate match, especially to the highest peaks.Comment: 12 pages, 10 figure

    Galaxy-galaxy weak-lensing measurement from SDSS: II. host halo properties of galaxy groups

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    As the second paper of a series on studying galaxy-galaxy lensing signals using the Sloan Digital Sky Survey Data Release 7 (SDSS DR7), we present our measurement and modelling of the lensing signals around groups of galaxies. We divide the groups into four halo mass bins, and measure the signals around four different halo-center tracers: brightest central galaxy (BCG), luminosity-weighted center, number-weighted center and X-ray peak position. For X-ray and SDSS DR7 cross identified groups, we further split the groups into low and high X-ray emission subsamples, both of which are assigned with two halo-center tracers, BCGs and X-ray peak positions. The galaxy-galaxy lensing signals show that BCGs, among the four candidates, are the best halo-center tracers. We model the lensing signals using a combination of four contributions: off-centered NFW host halo profile, sub-halo contribution, stellar contribution, and projected 2-halo term. We sample the posterior of 5 parameters i.e., halo mass, concentration, off-centering distance, sub halo mass, and fraction of subhalos via a MCMC package using the galaxy-galaxy lensing signals. After taking into account the sampling effects (e.g. Eddington bias), we found the best fit halo masses obtained from lensing signals are quite consistent with those obtained in the group catalog based on an abundance matching method, except in the lowest mass bin. Subject headings: (cosmology:) gravitational lensing, galaxies: clusters: generalComment: 12 pages, 7 figures, submitted to Ap
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