2008
DOI: 10.1086/592079
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An Ideal Mass Assignment Scheme for Measuring the Power Spectrum with Fast Fourier Transforms

Abstract: In measuring the power spectrum of the distribution of large numbers of dark matter particles in simulations, or galaxies in observations, one has to use fast Fourier transforms ( FFT) for calculational efficiency. However, because of the required mass assignment onto grid points in this method, the measured power spectrum hj f (k)j 2 i obtained with an FFT is not the true power spectrum P(k), but instead, one that is convolved with a window function jW (k)j 2 in Fourier space. In a recent paper, Jing proposed… Show more

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Cited by 53 publications
(62 citation statements)
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“…An alternative approach was taken by Cui et al (2008) who introduce the use of Daubechies wavelets to approximate the ideal filter while keeping compactness in position-space. We do not consider this technique here because the centre of mass of the wavelets adopted is offset from the particle position and so they are not well suited for estimation of the density field.…”
Section: Discussionmentioning
confidence: 99%
“…An alternative approach was taken by Cui et al (2008) who introduce the use of Daubechies wavelets to approximate the ideal filter while keeping compactness in position-space. We do not consider this technique here because the centre of mass of the wavelets adopted is offset from the particle position and so they are not well suited for estimation of the density field.…”
Section: Discussionmentioning
confidence: 99%
“…As we mentioned above, in underdense regions if the grid is made too fine there will be grid points for which no particle is assigned, which means there is no information on the velocity field, but typically one would set to zero (incorrectly) the velocity. In addition, dividing the interpolated momentum by the interpolated density means that it is difficult to correct for the interpolation kernel after the velocity field is Fourier transformed, unlike the case of the density field (see [45] for a recent discussion of interpolation corrections and comparison of CIC with other mass assignment schemes for the density field). We generate a Gaussian velocity field on a grid of 400 3 cells with a divergence and vorticity power spectra based roughly on expectations from previous measurements in the literature [46] and then interpolate this velocity on the positions of the 640 3 dark matter particles obtained from running an N-body simulation with Gadget2 [47] (see Table I below for more details on the simulations).…”
Section: Testing the Delaunay Methodsmentioning
confidence: 99%
“…For the power spectrum we used the nonlinear power spectrum from halofit Peacock & Smith (2000) adhering to the L500 cosmological parameters. In addition, to better match the real power spectrum in simulation we added Cloud-In-Cell window function Cui et al (2008) with a 2 h −1 Mpc smoothing kernel in the computation. We tune the free model parameters for weighted and unweighted c 11 respectively to better match the simulation results for the highest mass bin (upper line).…”
Section: Methodsmentioning
confidence: 99%