2007
DOI: 10.1137/040606715
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Projected Generalized Discrete-Time Periodic Lyapunov Equations and Balanced Realization of Periodic Descriptor Systems

Abstract: From the necessary and sufficient conditions for complete reachability and observability of periodic time-varying descriptor systems, the symmetric positive semi-definite reachability/observability Gramians are defined. These Gramians can be shown to satisfy some projected generalized discrete-time periodic Lyapunov equations. We propose a numerical method for solving these projected Lyapunov equations, and an illustrative numerical example is given. As an application of our results, the balanced realization o… Show more

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Cited by 38 publications
(45 citation statements)
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“…k=0 corresponding to the eigenvalue at infinity (Benner et al (2011b);Chu et al (2007);Stykel (2008)). This type of equations arises in the context of periodic state feedback problems and in model reduction of periodic descriptor systems when the solutions of the noncausal matrix equations associated with the systems (Kuo et al (2004);Benner et al (2011a);Chu et al (2007)) are sought.…”
Section: Preliminariesmentioning
confidence: 99%
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“…k=0 corresponding to the eigenvalue at infinity (Benner et al (2011b);Chu et al (2007);Stykel (2008)). This type of equations arises in the context of periodic state feedback problems and in model reduction of periodic descriptor systems when the solutions of the noncausal matrix equations associated with the systems (Kuo et al (2004);Benner et al (2011a);Chu et al (2007)) are sought.…”
Section: Preliminariesmentioning
confidence: 99%
“…This type of equations arises in the context of periodic state feedback problems and in model reduction of periodic descriptor systems when the solutions of the noncausal matrix equations associated with the systems (Kuo et al (2004);Benner et al (2011a);Chu et al (2007)) are sought. Note that in that case Q l (k) = I n −P l (k) and Q r (k) = I n − P r (k), where P l (k), P r (k) are the spectral projectors onto the k-th left and right deflating subspaces of the periodic matrix pairs {(E k , A k )} K−1 k=0 corresponding to the finite eigenvalues.…”
Section: Preliminariesmentioning
confidence: 99%
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