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306 3. Reference Manual<br />

3.8 Pole/Zero Analysis<br />

This chapter describes the Analog Insydes functions for numerical and symbolic pole/zero analysis<br />

by solving generalized eigenvalue problems (GEPs). The GEPs considered here have the form<br />

A ΛBu ⩵ <br />

v H A ΛB ⩵ <br />

where A and B are real-valued square matrices that arise from decomposing the coefficient matrix<br />

of a system of circuit equations Ts x ⩵ b into the contributions from the static and the dynamic<br />

elements.<br />

Ts ⩵ A sB<br />

In the above GEP, Λ is an eigenvalue, and u and v denote the right and left eigenvectors corresponding<br />

to Λ (v H denotes the Hermitian conjugate of v). In the following, the pairs Λ u and Λ v are referred<br />

to as (left and right) eigenpairs of the matrix pencil A B. Analog Insydes includes two different GEP<br />

solvers: an enhanced version of the QZ algorithm and a variant of the Jacobi orthogonal correction<br />

method (JOCM).<br />

The following table shows the available Analog Insydes functions for solving GEPs:<br />

GeneralizedEigensystem (Section 3.8.1)<br />

computing eigenvalues and eigenvectors by QZ<br />

GeneralizedEigenvalues (Section 3.8.2)<br />

computing eigenvalues by QZ<br />

PolesAndZerosByQZ (Section 3.8.3)<br />

computing poles and zeros by QZ<br />

PolesByQZ (Section 3.8.4)<br />

ZerosByQZ (Section 3.8.5)<br />

RootLocusByQZ (Section 3.8.6)<br />

LREigenpair (Section 3.8.7)<br />

computing poles by QZ<br />

computing zeros by QZ<br />

computing root locus by QZ<br />

computing eigenvalues and eigenvectors by JOCM

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