z-logo
open-access-imgOpen Access
Cosmological Perturbations: Entering the Nonlinear Regime
Author(s) -
Román Scoccimarro
Publication year - 1997
Publication title -
the astrophysical journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.376
H-Index - 489
eISSN - 1538-4357
pISSN - 0004-637X
DOI - 10.1086/304578
Subject(s) - bispectrum , physics , trispectrum , spectral density , perturbation theory (quantum mechanics) , skewness , nonlinear system , statistical physics , perturbation (astronomy) , gaussian , cosmological perturbation theory , quantum electrodynamics , mathematical physics , quantum mechanics , non gaussianity , mathematics , cosmology , statistics , anisotropy , cosmic microwave background
We consider one-loop corrections to the bispectrum and skewness ofcosmological density fluctuations induced by gravitational evolution. As hasbeen established by comparison with numerical simulations, tree-levelperturbation theory (PT) describes these quantities at the largest scales.One-loop PT provides a tool to probe the transition to the non-linear regime onsmaller scales. In this work, we find that, as a function of spectral index n,the one-loop bispectrum follows a pattern analogous to that of the one-looppower spectrum, which shows a change in behavior at a critical index n_c =-1.4, where non-linear corrections vanish. For the bispectrum, for n less thann_c, one-loop corrections increase the configuration dependence of the leadingorder contribution; for n greater than n_c, one-loop corrections tend to cancelthe configuration dependence of the tree-level bispectrum, in agreement withknown results from n=-1 numerical simulations. A similar situation is shown tohold for the Zel'dovich approximation (ZA), where n_c = -1.75. Usingdimensional regularization, we obtain explicit analytic expressions for theone-loop bispectrum for n=-2 initial power spectra, for both the exact dynamicsof gravitational instability and the ZA. We also compute the skewness factor,including local averaging of the density field, for n=-2: S_3(R) = 4.02 + 3.83sigma^2(R) for gaussian smoothing and S_3(R) = 3.86 + 3.18 sigma^2(R) fortop-hat smoothing, where sigma^2(R) is the variance of the density fieldfluctuations smoothed over a window of radius R. Comparison with fullynon-linear numerical simulations implies that, for n < -1, one-loop PT canextend our understanding of nonlinear clustering down to scales where thetransition to the stable clustering regime begins.Comment: 38 pages, 10 figures. Submitted to ApJ, August 199

The content you want is available to Zendy users.

Already have an account? Click here to sign in.
Having issues? You can contact us here
Accelerating Research

Address

John Eccles House
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom