Abstract

We study the asymptotic stability of non-autonomous linear systems with time dependent coefficient matrices { A ( t ) } t ∈ R . The classical theorem of Levinson has been an indispensable tool for the study of the asymptotic stability of non-autonomous linear systems. Contrary to constant coefficient system, having all eigenvalues in the left half complex plane does not imply asymptotic stability of the zero solution. Levinson’s theorem assumes that the coefficient matrix is a suitable perturbation of the diagonal matrix. Our objective is to prove a theorem similar to Levinson’s Theorem when the family of matrices merely admits an upper triangular factorization. In fact, in the presence of defective eigenvalues, Levinson’s Theorem does not apply. In our paper, we first investigate the asymptotic behavior of upper triangular systems and use the fixed point theory to draw a few conclusions. Unless stated otherwise, we aim to understand asymptotic behavior dimension by dimension, working with upper triangular with internal blocks adds flexibility to the analysis.

Highlights

  • We study the asymptotic stability of non-autonomous linear systems of ordinary differential equations x 0 ( t ) = A ( t ) x ( t ), (1)

  • For the reader’s convenience, we include the theorem in the Appendix. This classical theorem has been an indispensable tool in many science and engineering problems, giving the right asymptotic stability of a given system

  • We first consider the asymptotic stability when the coefficient is upper triangular. This result is used as the building blocks of the asymptotic stability of a larger system with blocks that are upper triangular

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Summary

Introduction

Non-autonomous linear systems typically arise when linearizing a non-linear dynamical system along a particular solution of interest that is not necessarily a fixed point In this case, the asymptotic stability of a linearized non-autonomous system is the linear stability of the solution of interest. For the reader’s convenience, we include the theorem in the Appendix This classical theorem has been an indispensable tool in many science and engineering problems, giving the right asymptotic stability of a given system. It ha been generalized in many different ways by the authors of [3,4,5,6,7].

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