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Proof of Maximum Flatness at DC

The maximumally flat fractional-delay FIR filter is obtained by equating to zero all $ N+1$ leading terms in the Taylor (Maclaurin) expansion of the frequency-response error at dc:

\begin{eqnarray*}
0 &=& \left.\frac{d^k}{d\omega^k} E(e^{j\omega}) \right\vert _...
...ert _{\omega=0}\\
&=& (-j\Delta)^k - \sum_{n=0}^N (-jn)^k h(n)
\end{eqnarray*}

$\displaystyle \,\,\Rightarrow\,\,\zbox {\sum_{n=0}^N n^k h(n) = \Delta^k, \; k=0,1,\ldots,N}
$

This is a linear system of equations of the form $ V\underline{h}=\underline{\Delta}$, where $ V$ is a Vandermonde matrix. The solution can be written as a ratio of Vandermonde determinants using Cramer's rule [336]. As shown by Cauchy (1812), the determinant of a Vandermonde matrix $ [p_i^{j-1}]$, $ i,j=1,\ldots,N$ can be expressed in closed form as

\begin{eqnarray*}
\left\vert\left[p_i^{j-1}\right]\right\vert &=& \prod_{j>i}(p_...
...dots\\
&&(p_{N-1}-p_{N-2})(p_N-p_{N-2})\cdot\\
&&(p_N-p_{N-1})
\end{eqnarray*}

Making this substitution in the solution obtained by Cremer's rule yields that the impulse response of the order $ N$ maximally flat fractional-delay FIR filter may be written in closed form as

$\displaystyle h(n) = \prod_{\stackrel{k=0}{k\ne n}}^N \frac{D-k}{n-k}
$

which coincides with the formula for Lagrange interpolation when the abscissae are equally spaced on the integers from 0 to $ N-1$.

Further details regarding the theory of Lagrange interpolation can be found (online) in [515, Ch. 3, Pt. 2, pp. 82-84].


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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.