4.7 Article

Near optimal bispectrum estimators for large-scale structure

Journal

PHYSICAL REVIEW D
Volume 91, Issue 4, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.91.043530

Keywords

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Funding

  1. Institute for Advanced Study through the Corning Glass Works Foundation Fellowship
  2. Office of Science of the U.S. Department of Energy [DE-AC02-05CH11231]
  3. BIS National E-infrastructure capital [ST/J005673/1]
  4. STFC [ST/H008586/1, ST/K00333X/1]
  5. STFC [ST/M00418X/1, ST/H008586/1, ST/J005673/1, ST/K00333X/1, ST/M007065/1] Funding Source: UKRI
  6. Science and Technology Facilities Council [ST/M007065/1, ST/K00333X/1, ST/J005673/1, ST/M00418X/1, ST/H008586/1] Funding Source: researchfish

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Clustering of large-scale structure provides significant cosmological information through the power spectrum of density perturbations. Additional information can be gained from higher-order statistics like the bispectrum, especially to break the degeneracy between the linear halo bias b(1) and the amplitude of fluctuations s(8). We propose new simple, computationally inexpensive bispectrum statistics that are near optimal for the specific applications like bias determination. Corresponding to the Legendre decomposition of nonlinear halo bias and gravitational coupling at second order, these statistics are given by the cross-spectra of the density with three quadratic fields: the squared density, a tidal term, and a shift term. For halos and galaxies the first two have associated nonlinear bias terms b(2) and b(s)(2), respectively, while the shift term has none in the absence of velocity bias (valid in the k -> 0 limit). Thus the linear bias b(1) is best determined by the shift cross-spectrum, while the squared density and tidal cross-spectra mostly tighten constraints on b(2) and b(s)(2) once b(1) is known. Since the form of the cross-spectra is derived from optimal maximum-likelihood estimation, they contain the full bispectrum information on bias parameters. Perturbative analytical predictions for their expectation values and covariances agree with simulations on large scales, k less than or similar to 0.09h/Mpc at z = 0.55 with Gaussian R = 20h(-1) Mpc smoothing, for matter-mattermatter, and matter-matter-halo combinations. For halo-halo-halo cross-spectra the model also needs to include corrections to the Poisson stochasticity.

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