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Poles of a State Space Filter
In this section, we show that the poles of a state-space model are given
by the eigenvalues of the state-transition matrix
.
Beginning again with the transfer function of the general state-space
model,
we may first observe that the poles of

are either the same as
or some subset of the poles of
(They are the same when all modes are
controllable and
observable [
37].)
By
Cramer's rule for matrix inversion, the denominator polynomial for

is given by the
determinant
where

denotes the
determinant of the square matrix

. (The determinant of

is also often written

.)
In
linear algebra, the polynomial

is called the
characteristic polynomial for the matrix

.
The roots of the characteristic polynomial are called the
eigenvalues of

.
Thus, the eigenvalues of the state transition matrix
are the
poles of the corresponding linear time-invariant system. In
particular, note that the poles of the system do not depend on the
matrices
, although these matrices, by placing system zeros,
can cause pole-zero cancellations (unobservable or uncontrollable
modes).
Previous:
Transposition of a State Space FilterNext:
Difference Equations to State Space
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.