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Flip Theorems

Let the flip operator be denoted by

\begin{eqnarray*}
\hbox{\sc Flip}_t(x) &\isdef & x(-t)\\
\hbox{\sc Flip}_\omega(X) &\isdef & X(-\omega),
\end{eqnarray*}

where $ t\in(-\infty,\infty)$ denotes time in seconds, and $ \omega\in(-\infty,\infty)$ denotes frequency in radians per second. The following Fourier pairs are easily verified:

\begin{eqnarray*}
\hbox{\sc Flip}(x) &\longleftrightarrow& \hbox{\sc Flip}(X)\\ ...
...\overline{x} &\longleftrightarrow& \hbox{\sc Flip}(\overline{X})
\end{eqnarray*}

The proof of the first relation is as follows:

\begin{eqnarray*}
\hbox{\sc FT}_{\omega}\left[\hbox{\sc Flip}(x)\right] &\isdef ...
...) \tau} d\tau\\
&=& X(-\omega) \isdef \hbox{\sc Flip}_\omega(X)
\end{eqnarray*}


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``Spectral Audio Signal Processing'', by Julius O. Smith III, (August 2008 Draft).
Copyright © 2008-08-13 by Julius O. Smith III
Center for Computer Research in Music and Acoustics (CCRMA),   Stanford University
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