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PSF and Weighted Overlap Add

Using ``square-root windows'' $ \sqrt{w}$ in the WOLA context, the valid hop sizes $ R$ are identical to those for $ w$ in the OLA case. More generally, given any window $ w(n)$ for use in a WOLA system, it is of interest to determine the hop sizes which yield perfect reconstruction.

Recall that, by the Poisson Summation Formula (PSF),

$\displaystyle \zbox {\underbrace{\sum_m w(n-mR)}_{\hbox{\sc Alias}_R(w)} = \und...
...e}_{\frac{2\pi}{R}}(W)\right]}} \quad \omega_k \isdef \frac{2\pi k}{R} \protect$

For WOLA, this is easily modified to become

$\displaystyle \zbox {\underbrace{\sum_m w(n-mR)f(n-mR)}_{\hbox{\sc Alias}_R(w\c...
...le}_{\frac{2\pi}{R}}(W\ast F)\right]}}
\quad \omega_k \isdef \frac{2\pi k}{R}
$

where $ w(n)$ is the analysis window and $ f(n)$ is the synthesis window.

When $ w=f$, this becomes

$\displaystyle \underbrace{\sum_m w^2(n-mR)}_{\hbox{\sc Alias}_R(w^2)} =
\under...
...ple}_{\frac{2\pi}{R}}(W\ast W)\right]},
\quad \omega_k \isdef \frac{2\pi k}{R}
$


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Previous: PSF Dual and Graphical Equalizers
Next: Example COLA Windows for WOLA

written by Julius Orion Smith III
Julius Smith's background is in electrical engineering (BS Rice 1975, PhD Stanford 1983). He is presently Professor of Music and Associate Professor (by courtesy) of Electrical Engineering at Stanford's Center for Computer Research in Music and Acoustics (CCRMA), teaching courses and pursuing research related to signal processing applied to music and audio systems. See http://ccrma.stanford.edu/~jos/ for details.


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