Because of mass assignment onto grid points in the measurement of the power spectrum using a fast Fourier transform (FFT), the raw power spectrum ⟨|δf(k)|2⟩ estimated with the FFT is not the same as the true power spectrum P(k). In this paper we derive a formula that relates ⟨|δf(k)|2⟩ to P(k). For a sample of N discrete objects, the formula reads ⟨|δf(k)|2⟩ = [|W( + 2kN)|2P( + 2kN) + 1/N|W( + 2kN)|2], where W(k) is the Fourier transform of the mass assignment function W(r), kN is the Nyquist wavenumber, and n is an integer vector. The formula is different from that in some previous works in which the summation over n is neglected. For the nearest grid point, cloud-in-cell, and triangular-shaped cloud assignment functions, we show that the shot-noise term |W( + 2kN)|2 can be expressed by simple analytical functions. To reconstruct P(k) from the alias sum |W( + 2kN)|2P( + 2kN), we propose an iterative method. We test the method by applying it to an N-body simulation sample and show that the method can successfully recover P(k). The discussion is further generalized to samples with observational selection effects.
Correcting for the Alias Effect When Measuring the Power Spectrum Using a Fast Fourier Transform
Published 2004 in The Astrophysical Journal
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- Publication year
2004
- Venue
The Astrophysical Journal
- Publication date
2004-09-10
- Fields of study
Physics
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