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  4. An optical observational cluster mass function at z ∼1 with the ORELSE survey
 
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An optical observational cluster mass function at z ∼1 with the ORELSE survey

Journal
Monthly Notices of the Royal Astronomical Society
Journal Volume
502
Journal Issue
3
Pages
3942-3954
Date Issued
2021
Author(s)
Hung D
Lemaux B.C
Gal R.R
Tomczak A.R
Lubin L.M
Cucciati O
Pelliccia D
Shen L
Le Fèvre O
Zamorani G
PO-FENG WU  
Kocevski D.D
Fassnacht C.D
Squires G.K.
DOI
10.1093/mnras/stab300
URI
https://www.scopus.com/inward/record.uri?eid=2-s2.0-85117517668&doi=10.1093%2fmnras%2fstab300&partnerID=40&md5=cfc52ec02be9f50f2483ecc8ec92a469
https://scholars.lib.ntu.edu.tw/handle/123456789/624907
Abstract
We present a new mass function of galaxy clusters and groups using optical/near-infrared (NIR) wavelength spectroscopic and photometric data from the Observations of Redshift Evolution in Large-Scale Environments (ORELSE) survey. At z ∼1, cluster mass function studies are rare regardless of wavelength and have never been attempted from an optical/NIR perspective. This work serves as a proof of concept that z ∼1 cluster mass functions are achievable without supplemental X-ray or Sunyaev-Zel'dovich data. Measurements of the cluster mass function provide important contraints on cosmological parameters and are complementary to other probes. With ORELSE, a new cluster finding technique based on Voronoi tessellation Monte Carlo (VMC) mapping, and rigorous purity and completeness testing, we have obtained ∼240 galaxy overdensity candidates in the redshift range 0.55 < z < 1.37 at a mass range of 13.6 < log (M/M·) < 14.8. This mass range is comparable to existing optical cluster mass function studies for the local universe. Our candidate numbers vary based on the choice of multiple input parameters related to detection and characterization in our cluster finding algorithm, which we incorporated into the mass function analysis through a Monte Carlo scheme. We find cosmological constraints on the matter density, ωm, and the amplitude of fluctuations, σ8, of Ω m = 0.250+0.104-0.099 and σ 8 = 1.150+0.260-0.163. While our ωm value is close to concordance, our σ8 value is ∼2σ higher because of the inflated observed number densities compared to theoretical mass function models owing to how our survey targeted overdense regions. With Euclid and several other large, unbiased optical surveys on the horizon, VMC mapping will enable optical/NIR cluster cosmology at redshifts much higher than what has been possible before. © 2021 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society.
Subjects
cosmological parameters; galaxies: clusters: general; galaxies: groups: general; large-scale structure of Universe; techniques: photometric; techniques: spectroscopic
Type
journal article

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