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One Sine and One Cosine
(``Phase Quadrature'' Case)
All Four Resolutions Overlaid


\begin{psfrags}\psfrag{Frequency wT (rad/sample)}{
Frequency $\omega T$\ (rad/sample)}\psfrag{w}{\footnotesize $\omega$}\begin{center}
\epsfig{file=eps/resolvedSinesC2C.eps,width=6in} \\
\end{center} % unnormalized, uses legend
\end{psfrags}

The preceding figures suggest that, for a rectangular window of length $ M$ , two sinusoids can be most reliably resolved when they are separated in frequency by a full main-lobe width:

$\displaystyle \zbox{\Delta\omega\geq 2\Omega_M} \qquad \left(\Omega_M \isdef \frac{2\pi}{M}\right)
$

This implies there must be at least two full cycles of the difference-frequency under the window.

We'll see later that this is an overly conservative requirement--a more careful study reveals that $ 1.44$ cycles is sufficient for the rectangular window.


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``Music 421 Overview'', by Julius O. Smith III, (From Lecture Overheads, Music 421).
Copyright © 2020-06-27 by Julius O. Smith III
Center for Computer Research in Music and Acoustics (CCRMA),   Stanford University
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