Assembly bias in the local PNG halo bias and its implication for fNLf_{\rm NL} constraints

preprint2023arXivOpen access

Abstract

We use NN-body simulations to study halo assembly bias (i.e., the dependence of halo clustering on properties beyond total mass) in the density and primordial non-Gaussianity (PNG) linear bias parameters b1b_1 and bϕb_ϕ, respectively. We consider concentration, spin and sphericity as secondary halo properties, for which we find a clear detection of assembly bias for b1b_1 and bϕb_ϕ. At fixed total mass, halo spin and sphericity impact b1b_1 and bϕb_ϕ in a similar manner, roughly preserving the shape of the linear bϕ(b1)b_ϕ(b_1) relation satisfied by the global halo population. Halo concentration, however, drives b1b_1 and bϕb_ϕ in opposite directions. This induces significant changes to the bϕ(b1)b_ϕ(b_1) relation, with higher concentration halos having higher amplitude of bϕ(b1)b_ϕ(b_1). For z=0.5z=0.5 and b1≈2b_1 \approx 2 in particular, the population comprising either all halos, those with the 33%33\% lowest or those with the 33%33\% highest concentrations have a PNG bias of bϕ≈3b_ϕ\approx 3, bϕ≈−1b_ϕ\approx -1 and bϕ≈9b_ϕ\approx 9, respectively. Varying the halo concentration can make bϕb_ϕ very small and even change its sign. These results have important ramifications for galaxy clustering constraints of the local PNG parameter fNLf_{\rm NL} that assume fixed forms for the bϕ(b1)b_ϕ(b_1) relation. We illustrate the significant impact of halo assembly bias in actual data using the BOSS DR12 galaxy power spectrum: assuming that BOSS galaxies are representative of all halos, the 33%33\% lowest or the 33%33\% highest concentration halos yields σfNL=44,165,19σ_{f_{\rm NL}} = 44, 165, 19, respectively. Our results suggest taking host halo concentration into account in galaxy selection strategies to maximize the signal-to-noise on fNLf_{\rm NL}. They also motivate more simulation-based efforts to study the bϕ(b1)b_ϕ(b_1) relation of halos and galaxies.

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