Evolution of skewness and kurtosis of cosmic density fields
arXiv:2011.13292 · doi:10.1051/0004-6361/202039999
Abstract
Methods. We perform numerical simulations of the evolution of the cosmic web for the conventional LCDM model. The simulations cover a wide range of box sizes L = 256 - 4000 Mpc/h, mass and force resolutions and epochs from very early moments z = 30 to the present moment z = 0. We calculate density fields with various smoothing lengths to find the dependence of the density field on smoothing scale. We calculate PDF and its moments - variance, skewness and kurtosis. Results. We focus on the third (skewness S) and fourth (kurtosis K) moments of the distribution functions: their dependence on the smoothing scale, the amplitude of fluctuations and the redshift. During the evolution the reduced skewness and reduced kurtosis present a complex behaviour: at a fixed redshift curves of and steeply increase with at and then flatten out and become constant at . If we fix the smoothing scale , then after reaching the maximum at , the curves at large start to gradually decline. We provide accurate fits for the evolution of . Skewness and kurtosis approach at early epochs constant levels, depending on smoothing length: and . Conclusions. Most of statistics of dark matter clustering (e.g., halo mass function or concentration-mass relation) are nearly universal: they mostly depend on the with the relatively modest correction to explicit dependence on the redshift. We find just the opposite for skewness and kurtosis: the dependence of moments on evolutionary epoch and smoothing length is very different, together they determine the evolution of uniquely. The evolution of and cannot be described by current theoretical approximations.
arXiv comment17 pages, 14 figures, revised version accepted by Astronomy and Astrophysics
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