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Let bt denote a filter.
Then at is its inverse filter
if the convolution of at with bt is an impulse function.
In terms of Z-transforms,
an inverse is simply defined by A(Z) = 1/B(Z).
Whether the filter A(Z) is causal
depends on whether it is finite everywhere inside the unit circle,
or really on whether B(Z) vanishes
anywhere
inside the circle.
For example, B(Z)=1-2Z vanishes at Z = 1/2.
There A(Z)=1/B(Z) must be infinite,
that is to say,
the series A(Z) must be nonconvergent at Z = 1/2.
Thus, as we have just seen, at is noncausal.
A most interesting case, called
``minimum phase,"
occurs when both a filter B(Z) and its inverse are causal.
In summary,
causal: for causal inverse: for
minimum phase: both above conditions
The reason the interesting words ``minimum phase'' are used
is given in chapter .
Next: Mechanical interpretation
Up: Z-plane, causality, and feedback
Previous: Causality and the unit
Stanford Exploration Project
10/21/1998