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246 Chapter 6 IMPLEMENTATION OF DISCRETE-TIME FILTERS<br />

FIGURE 6.22<br />

Lattice-ladder structure for realizing a pole-zero IIR filter<br />

where {C m } are called the ladder coefficients that determine the zeros of<br />

the system function H(z). It can be shown [23] that {C m } are given by<br />

M∑<br />

B M (z) = C m J m (z) (6.26)<br />

m=0<br />

where J m (z) isthe polynomial in (6.20). From (6.26) one can obtain a<br />

recursive relation<br />

B m (z) =B m−1 (z)+C m J m (z);<br />

m =1, 2,...,M<br />

or equivalently,<br />

M∑<br />

C m = b m + C i α i (i − m); m = M, M − 1,...,0 (6.27)<br />

i=m+1<br />

from the definitions of B m (z) and A m (z).<br />

6.4.6 MATLAB IMPLEMENTATION<br />

To obtain a lattice-ladder structure for a general rational IIR filter, we<br />

can first obtain the lattice coefficients {K m } from A N (z) using the recursion<br />

(6.20). Then we can solve (6.27) recursively for the ladder coefficients<br />

{C m } to realize the numerator B M (z). This is done in the following<br />

MATLAB function dir2ladr.Itcan also be used to determine the all-pole<br />

lattice parameters when the array b is set to b=[1].<br />

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