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Repeat (Scaling) Operator

We define the repeat operator in the frequency domain as a scaling of frequency axis by some integer factor $ L>0$:

$\displaystyle \hbox{\sc Repeat}_{L,\nu}(X) \isdef X(L\omega), \quad \omega\in\left[-\frac{\pi}{L},\frac{\pi}{L}\right],
$

where $ \nu=L\omega\in[-\pi,\pi)$ denotes the radian frequency variable after applying the repeat operator.

The repeat operator maps the entire unit circle (taken as $ -\pi$ to $ \pi$) to a segment of itself $ [-\pi/L,\pi/L]$, centered about $ \omega
= 0$, and repeated $ L$ times. This is illustrated in Fig.2.2 for $ L=3$.


\begin{psfrags}
% latex2html id marker 8268\psfrag{t}{\normalsize $\omega$}...
...at2}
\caption{Illustration of the repeat operator.}
\end{figure}
\end{psfrags}

Since the frequency axis is continuous and $ 2\pi$-periodic for DTFTs, the repeat operator is precisely equivalent to a scaling operator for the Fourier transform case (§2.4.4). We call it ``repeat'' rather than ``scale'' because we are restricting the scale factor to positive integers, and because the name ``repeat'' describes more vividly what happens to a periodic spectrum that is compressively frequency-scaled over the unit circle.


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Previous: Stretch Operator
Next: Stretch/Repeat (Scaling) Theorem

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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