Quijote-PNG: The Information Content of the Halo Mass Function

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Hauptverfasser: Jung, Gabriel, Ravenni, Andrea, Baldi, Marco, Coulton, William R., Jamieson, Drew, Karagiannis, Dionysios, Liguori, Michele, Shao, Helen, Verde, Licia, Villaescusa-Navarro, Francisco, Wandelt, Benjamin D.
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Veröffentlicht: 2023
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author Jung, Gabriel
Ravenni, Andrea
Baldi, Marco
Coulton, William R.
Jamieson, Drew
Karagiannis, Dionysios
Liguori, Michele
Shao, Helen
Verde, Licia
Villaescusa-Navarro, Francisco
Wandelt, Benjamin D.
author_facet Jung, Gabriel
Ravenni, Andrea
Baldi, Marco
Coulton, William R.
Jamieson, Drew
Karagiannis, Dionysios
Liguori, Michele
Shao, Helen
Verde, Licia
Villaescusa-Navarro, Francisco
Wandelt, Benjamin D.
contents We study signatures of primordial non-Gaussianity (PNG) in the redshift-space halo field on non-linear scales, using a combination of three summary statistics, namely the halo mass function (HMF), power spectrum, and bispectrum. The choice of adding the HMF to our previous joint analysis of power spectrum and bispectrum is driven by a preliminary field-level analysis, in which we train graph neural networks on halo catalogues to infer the PNG $f_\mathrm{NL}$ parameter. The covariance matrix and the responses of our summaries to changes in model parameters are extracted from a suite of halo catalogues constructed from the Quijote-PNG N-body simulations. We consider the three main types of PNG: local, equilateral and orthogonal. Adding the HMF to our previous joint analysis of power spectrum and bispectrum produces two main effects. First, it reduces the equilateral $f_\mathrm{NL}$ predicted errors by roughly a factor $2$, while also producing notable, although smaller, improvements for orthogonal PNG. Second, it helps break the degeneracy between the local PNG amplitude, $f_\mathrm{NL}^\mathrm{local}$, and assembly bias, $b_ϕ$, without relying on any external prior assumption. Our final forecasts for PNG parameters are $Δf_\mathrm{NL}^\mathrm{local} = 40$, $Δf_\mathrm{NL}^\mathrm{equil} = 210$, $Δf_\mathrm{NL}^\mathrm{ortho} = 91$, on a cubic volume of $1 \left(h^{-1}{\rm Gpc}\right)^3$, with a halo number density of $\bar{n}\sim 5.1 \times 10^{-5}~h^3\mathrm{Mpc}^{-3}$, at $z = 1$, and considering scales up to $k_\mathrm{max} = 0.5~h\,\mathrm{Mpc}^{-1}$.
format Preprint
id arxiv_https___arxiv_org_abs_2305_10597
institution arXiv
publishDate 2023
record_format arxiv
spellingShingle Quijote-PNG: The Information Content of the Halo Mass Function
Jung, Gabriel
Ravenni, Andrea
Baldi, Marco
Coulton, William R.
Jamieson, Drew
Karagiannis, Dionysios
Liguori, Michele
Shao, Helen
Verde, Licia
Villaescusa-Navarro, Francisco
Wandelt, Benjamin D.
Cosmology and Nongalactic Astrophysics
We study signatures of primordial non-Gaussianity (PNG) in the redshift-space halo field on non-linear scales, using a combination of three summary statistics, namely the halo mass function (HMF), power spectrum, and bispectrum. The choice of adding the HMF to our previous joint analysis of power spectrum and bispectrum is driven by a preliminary field-level analysis, in which we train graph neural networks on halo catalogues to infer the PNG $f_\mathrm{NL}$ parameter. The covariance matrix and the responses of our summaries to changes in model parameters are extracted from a suite of halo catalogues constructed from the Quijote-PNG N-body simulations. We consider the three main types of PNG: local, equilateral and orthogonal. Adding the HMF to our previous joint analysis of power spectrum and bispectrum produces two main effects. First, it reduces the equilateral $f_\mathrm{NL}$ predicted errors by roughly a factor $2$, while also producing notable, although smaller, improvements for orthogonal PNG. Second, it helps break the degeneracy between the local PNG amplitude, $f_\mathrm{NL}^\mathrm{local}$, and assembly bias, $b_ϕ$, without relying on any external prior assumption. Our final forecasts for PNG parameters are $Δf_\mathrm{NL}^\mathrm{local} = 40$, $Δf_\mathrm{NL}^\mathrm{equil} = 210$, $Δf_\mathrm{NL}^\mathrm{ortho} = 91$, on a cubic volume of $1 \left(h^{-1}{\rm Gpc}\right)^3$, with a halo number density of $\bar{n}\sim 5.1 \times 10^{-5}~h^3\mathrm{Mpc}^{-3}$, at $z = 1$, and considering scales up to $k_\mathrm{max} = 0.5~h\,\mathrm{Mpc}^{-1}$.
title Quijote-PNG: The Information Content of the Halo Mass Function
topic Cosmology and Nongalactic Astrophysics
url https://arxiv.org/abs/2305.10597