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Discreteness effects in simulations of hot/warm dark matter
Author(s) -
Wang Jie,
White Simon D. M.
Publication year - 2007
Publication title -
monthly notices of the royal astronomical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.058
H-Index - 383
eISSN - 1365-2966
pISSN - 0035-8711
DOI - 10.1111/j.1365-2966.2007.12053.x
Subject(s) - physics , matter power spectrum , dark matter , lattice (music) , computational physics , structure formation , astrophysics , wavenumber , wavelength , spurious relationship , mechanics , cosmology , optics , dark energy , machine learning , galaxy , acoustics , computer science
In hot/warm dark matter (HDM/WDM) universes the density fluctuations at early times contain very little power below a characteristic wavelength related inversely to the particle mass. We study how discreteness noise influences the growth of non‐linear structures smaller than this coherence scale in N ‐body simulations of cosmic structure formation. It has been known for 20 yr that HDM simulations in which the initial uniform particle load is a cubic lattice exhibit artefacts related to this lattice. In particular, the filaments which form in such simulations break up into regularly spaced clumps which reflect the initial grid pattern. We demonstrate that a similar artefact is present even when the initial uniform particle load is not a lattice, but rather a glass with no preferred directions and no long‐range coherence. Such regular fragmentation also occurs in simulations of the collapse of idealized, uniform filaments, although not in simulations of the collapse of infinite uniform sheets. In HDM or WDM simulations all self‐bound non‐linear structures with masses much smaller than the free streaming mass appear to originate through spurious fragmentation of filaments. These artificial fragments form below a characteristic mass which scales as m 1/3 p k −2 peak , where m p is the N ‐body particle mass and k peak is the wavenumber at the maximum of k 3 P ( k )[ P ( k ) is the power spectrum]. This has the unfortunate consequence that the effective mass resolution of such simulations improves only as the cube root of the number of particles employed.

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