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◆ Journal of Cosmology and Astroparticle Physics2026-02-01· Physics

Modeling and measuring the anisotropic halo 3-point correlation function: a coordinated study

A. Farina, A. Veropalumbo, E. Branchini, M. Guidi

原始摘要(英文原文)· Original abstract
Abstract Apparent anisotropies in the statistical properties of the spatial distribution of galaxies encode precious cosmological information. Its extraction is commonly performed using 2-point clustering statistics. However, ongoing and future spectroscopic galaxy surveys will cover unprecedented volumes with a number of objects large enough to effectively probe clustering anisotropies through higher-order statistics. In this work, we present a novel and efficient implementation of both a model for the multipole moments of the anisotropic 3-point correlation function (3PCF) and of their estimator. To evaluate the performance of our model, we compared its predictions against 3PCF measurements obtained with our estimator from a set of 298 dark matter halo catalogs drawn from the z = 1 snapshots of N -body simulations. For the statistical analysis, we employed a covariance matrix estimated from an independent suite of 3000 mock halo catalogs at the same redshift. We then repeated the analysis by combining the 2-point correlation function (2PCF) to the 3PCF, with and without including its anisotropic part. In the 3PCF-only analysis, the addition of the anisotropic component of the 3PCF effectively breaks the degeneracy between the growth rate f and the linear bias b 1 , significantly reducing their uncertainties. It also significantly improves the precision of the Alcock-Paczynski parameter ε but does not reduce the ∼ 1 % offset we find in the estimate of the isotropic dilation parameter α . The joint 2PCF+3PCF analysis reduces, though does not fully remove, biases in the AP and isotropic dilation parameters and breaks the f - b 1 - σ 8 degeneracy, leading to tighter constraints overall. The anisotropic 3PCF adds little to the joint analysis because the tree-level 3PCF model fails to capture the anisotropic information primarily encoded on small scales and in squeezed triangle configurations. A more advanced model, e.g. based on 1-loop perturbation theory, will be required to exploit this information fully.
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