Next  |  Prev  |  Up  |  Top  |  JOS Index  |  JOS Pubs  |  JOS Home  |  Search

Proof of Downsampling/Aliasing Relationship


$\displaystyle \zbox{\hbox{\sc Downsample}_N(x) \leftrightarrow \frac{1}{N} \hbox{\sc Alias}_N(X)}
$

or         \fbox{$x(nN) \leftrightarrow \frac{1}{N} \displaystyle\sum_{m=0}^{N-1} X\left(e^{j2\pi m/N} z^{1/N}\right)$}

From the DFT case, we know this is true when $ x$ and $ X$ are each complex sequences of length $ N_s$ , in which case $ y$ and $ Y$ are length $ N_s/N$ . Thus,

$\displaystyle x(nN) \leftrightarrow
Y(\omega_k N) = \frac{1}{N} \sum_{m=0}^{N-1} X\left(\omega_k + \frac{2\pi}{N} m \right), \; k\in \left[0,\frac{N_s}{N}\right)
$

where we have chosen to keep frequency samples $ \omega_k$ in terms of the original frequency axis prior to downsampling, i.e., $ \omega_k =
2\pi k/ N_s$ for both $ X$ and $ Y$ . This choice allows us to easily take the limit as $ N_s\to\infty$ by simply replacing $ \omega_k$ by $ \omega$ :

$\displaystyle x(nN) \leftrightarrow
Y(\omega N) = \frac{1}{N} \sum_{m=0}^{N-1} X\left(\omega + \frac{2\pi}{N} m \right), \; \omega\in\left[0,\frac{2\pi}{N}\right)
$

Replacing $ \omega$ by $ \omega^\prime =\omega N$ and converting to $ z$ -transform notation $ X(z)$ instead of Fourier transform notation $ X(\omega)$ , with $ z=e^{j\omega^\prime }$ , yields the final result.


Next  |  Prev  |  Up  |  Top  |  JOS Index  |  JOS Pubs  |  JOS Home  |  Search

Download JFB.pdf
Download JFB_2up.pdf
Download JFB_4up.pdf
[Comment on this page via email]

``Multirate, Polyphase, and Wavelet Filter Banks'', by Julius O. Smith III, Scott Levine, and Harvey Thornburg, (From Lecture Overheads, Music 421).
Copyright © 2020-06-02 by Julius O. Smith III, Scott Levine, and Harvey Thornburg
Center for Computer Research in Music and Acoustics (CCRMA),   Stanford University
CCRMA  [Automatic-links disclaimer]