2018
DOI: 10.1093/mnras/sty463
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The Santiago–Harvard–Edinburgh–Durham void comparison – I. SHEDding light on chameleon gravity tests

Abstract: We present a systematic comparison of several existing and new void finding algorithms, focusing on their potential power to test a particular class of modified gravity modelschameleon f (R) gravity. These models deviate from standard General Relativity (GR) more strongly in low-density regions and thus voids are a promising venue to test them. We use Halo Occupation Distribution (HOD) prescriptions to populate haloes with galaxies, and tune the HOD parameters such that the galaxy two-point correlation functio… Show more

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Cited by 125 publications
(179 citation statements)
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“…In this section, we briefly introduce the N-body simulations we will use to assess the performance of our analytical model, which is a crucial step for our analysis. The first set of simulations, that we will refer to from now on as Group I simulations, are the Extended LEnsing PHysics using ANalaytic ray Tracing (ELEPHANT) simulations [94], that were performed with two modified versions of the GR code (RAMSES): the ECOSMOG module [95,96] produced snapshots for the F6, F5 and F4 cases at a cosmological redshift of z = 0.5, while ECOSMOG-V [97][98][99] was used to produce the nDGP N1 and N5 realizations, also at z = 0.5. 1024 3 dark matter particles were evolved, in a simulation box with a side L box = 1024M pc/h and a cosmology specified by the following parameters:…”
Section: N-body Simulationsmentioning
confidence: 99%
“…In this section, we briefly introduce the N-body simulations we will use to assess the performance of our analytical model, which is a crucial step for our analysis. The first set of simulations, that we will refer to from now on as Group I simulations, are the Extended LEnsing PHysics using ANalaytic ray Tracing (ELEPHANT) simulations [94], that were performed with two modified versions of the GR code (RAMSES): the ECOSMOG module [95,96] produced snapshots for the F6, F5 and F4 cases at a cosmological redshift of z = 0.5, while ECOSMOG-V [97][98][99] was used to produce the nDGP N1 and N5 realizations, also at z = 0.5. 1024 3 dark matter particles were evolved, in a simulation box with a side L box = 1024M pc/h and a cosmology specified by the following parameters:…”
Section: N-body Simulationsmentioning
confidence: 99%
“…However, the choice is not yet completely ruled out by cosmological observations, and for the GGL analysis we would like to choose a model that can maximize the difference from GR (see e.g. Cai, Padilla & Li 2015;Cataneo et al 2015;Liu et al 2016;Shirasaki, Hamana & Yoshida 2016;Shirasaki et al 2017;Peirone et al 2017;Cautun et al 2017, for some recent studies on the current and potential constraints f(R) gravity).…”
Section: The Choice Of F(r) Modelmentioning
confidence: 99%
“…For GGL, we have assumed the lens galaxies are at z lens = 0.30. as LSST (see e.g. Cautun et al 2017, for some relevant S/N analysis but for void lensing using Euclid and LSST). For simplicity, let us assume that there are overlapping spectroscopic surveys which can provide galaxy catalogues with a number density at least as high as the ones used in our lensing galaxies, between 0.16 z 0.43.…”
Section: The Excess Surface Density Profilesmentioning
confidence: 99%
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“…Our basic concept is to (1) split the sky by the count of tracer galaxies in a top-hat aperture and extended redshift range into quantiles of density, and to (2) measure the gravitational shear around each of the quantiles to reconstruct the matter density PDF. These measurements are a generalization of trough lensing, introduced in Gruen et al [23] (see also [24][25][26]). They are also closely related to the galaxy-matter aperture statistics of Simon et al [27].…”
Section: Introductionmentioning
confidence: 99%