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<i>Euclid</i>preparation

A. PezzottaClaudio MorettiMatteo ZennaroAzadeh Moradinezhad DizgahM. CrocceE. SefusattiI. FerreroKevin PardedeAlexander EggemeierAlexandre BarreiraRaúl E. AnguloMarco MarinucciB. Camacho QuevedoS. de la TorreLAM - Laboratoire d'Astrophysique de Marseille (Pôle de l'Étoile Site de Château-Gombert 38, rue Frédéric Joliot-Curie 13388 Marseille cedex 13 - France)D. AlkhanishviliMatteo BiagettiMichel-Andrès BretonLUTH (UMR_8102) - Laboratoire Univers et Théories (5 place Jules Janssen 92195 Meudon cedex - France)Emanuele CastorinaGuido D’AmicoVincent DesjacquesM. GuidiM. KärcherLAM - Laboratoire d'Astrophysique de Marseille (Pôle de l'Étoile Site de Château-Gombert 38, rue Frédéric Joliot-Curie 13388 Marseille cedex 13 - France)Andrea OddoMarcos Pellejero-IbáñezC. PorcianiA. PugnoJ. SalvalaggioE SarpaA. VeropalumboZ. VlahA AmaraS. AndreonN. AuricchioMarco BaldiS. BardelliR. BenderC. BodendorfD. BoninoE. BranchiniM. BresciaJ. BrinchmannS. CameraV. CapobiancoC. CarboneV. F. CardoneJ. CarreteroSantiago CasasF. J. CastanderM. CastellanoS. CavuotiA. CimattiG. CongedoChristopher J. ConseliceL. ConversiY. CopinIP2I Lyon - Institut de Physique des 2 Infinis de Lyon (Campus LyonTech-la Doua Bâtiment Paul DIRAC 4 Rue Enrico Fermi 69622 Villeurbanne Cedex - France)L. CorcioneF. CourbinH. M. CourtoisIP2I Lyon - Institut de Physique des 2 Infinis de Lyon (Campus LyonTech-la Doua Bâtiment Paul DIRAC 4 Rue Enrico Fermi 69622 Villeurbanne Cedex - France)A. Da SilvaH. DegaudenziA. M. Di GiorgioJ. DinisX. DupacS. DusiniA. EaletIP2I Lyon - Institut de Physique des 2 Infinis de Lyon (Campus LyonTech-la Doua Bâtiment Paul DIRAC 4 Rue Enrico Fermi 69622 Villeurbanne Cedex - France)M. FarinaS. FarrensAIM (UMR7158 / UMR_E_9005 / UM_112) - Astrophysique Interprétation Modélisation (AIM - UMR 7158 - UMR E 9005, ex 'Astrophysique Interactions Multi-échelles', Service d'astrophysique, CEA/Saclay, Orme des Merisiers F-91191 GIF SUR YVETTE CEDEX - France)P. FosalbaM. FrailisE. FranceschiS. GaleottaB. GillisC. GiocoliB. R. GranettA. GrazianF. GruppL. GuzzoS. V. H. HauganF. HormuthA. HornstrupK. JahnkęB. JoachimiE. KeihänenS. KermicheCPPM - Centre de Physique des Particules de Marseille (163, avenue de Luminy - Case 902 - 13288 Marseille cedex 09 - France)A. KiesslingM. KilbingerCEA Paris-SaclayT. KitchingB. KubikIP2I Lyon - Institut de Physique des 2 Infinis de Lyon (Campus LyonTech-la Doua Bâtiment Paul DIRAC 4 Rue Enrico Fermi 69622 Villeurbanne Cedex - France)M. KunzH. Kurki‐SuonioS. LigoriP. B. LiljeV. LindholmI. LloroE. MaioranoO. MansuttiO. MarggrafK. MarkovičN. MartinetLAM - Laboratoire d'Astrophysique de Marseille (Pôle de l'Étoile Site de Château-Gombert 38, rue Frédéric Joliot-Curie 13388 Marseille cedex 13 - France)F. Marulli
2024en
ABI

Abstract

We investigate the accuracy of the perturbative galaxy bias expansion in view of the forthcoming analysis of the Euclid spectroscopic galaxy samples. We compare the performance of a Eulerian galaxy bias expansion using state-of-the-art prescriptions from the effective field theory of large-scale structure (EFTofLSS) with a hybrid approach based on Lagrangian perturbation theory and high-resolution simulations. These models are benchmarked against comoving snapshots of the flagship I N -body simulation at z = (0.9, 1.2, 1.5, 1.8), which have been populated with H α galaxies leading to catalogues of millions of objects within a volume of about 58 h −3 Gpc 3 . Our analysis suggests that both models can be used to provide a robust inference of the parameters ( h , ω c ) in the redshift range under consideration, with comparable constraining power. We additionally determine the range of validity of the EFTofLSS model in terms of scale cuts and model degrees of freedom. From these tests, it emerges that the standard third-order Eulerian bias expansion – which includes local and non-local bias parameters, a matter counter term, and a correction to the shot-noise contribution – can accurately describe the full shape of the real-space galaxy power spectrum up to the maximum wavenumber of k max = 0.45 h Mpc −1 , and with a measurement precision of well below the percentage level. Fixing either of the tidal bias parameters to physically motivated relations still leads to unbiased cosmological constraints, and helps in reducing the severity of projection effects due to the large dimensionality of the model. We finally show how we repeated our analysis assuming a volume that matches the expected footprint of Euclid , but without considering observational effects, such as purity and completeness, showing that we can get constraints on the combination ( h , ω c ) that are consistent with the fiducial values to better than the 68% confidence interval over this range of scales and redshifts.

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Cited by 20 references