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Nonlinear Modifications

In Fourier terms, the simplest nonlinearity is a square law. Consider an FFT processor that squares each frame spectrum:

$\displaystyle Y_m(\omega_k) = X_m^2(\omega_k)
$

In the time domain, each frame is convolved with itself:

$\displaystyle y_m(n) = (x_m*x_m)(n)
$

Since $ x_m$ is time limited to $ M$ samples, we can avoid time domain aliasing by requiring $ N \ge 2M-1$.

More generally, we can consider

$\displaystyle Y_m(\omega_k) = X_m^l(\omega_k).
$

This can be thought of as $ l$ cascaded convolutions of $ x_m$ with itself. The resulting signal will be at most $ l(M-l)+1$ samples long. We can avoid time domain aliasing in this case by requiring

$\displaystyle N \ge l(M-1)+1.
$

We can express a general class of nonlinearities as a polynomial in the spectrum:

$\displaystyle Y_m(\omega_k) = \sum_l^{K-1} \alpha_l X_m^l(\omega_k)
$

In this case, we require $ N \ge K(M-1)+1$ to avoid time aliasing.

For related information, look into Volterra series expansions [21]. The interated-convolution expansion above can be regarded as a special case of a Volterra series expansion.


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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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